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Nonuniqueness problems in numerical methods J T Chen( 陳正宗 ) Life-time Distinguished Prof
Taiwan Ocean University
August 8 1100-1200 2008
高海大旗津校區 高雄
(CFD15-2008-chenppt)
National Taiwan Ocean UniversityMSVLAB ( 海大河工系 )
Department of Harbor and River Engineering
2
Overview of numerical methods ( 中醫式的工程分析法 ) Nonuniqueness problems - review
BEM failure (mathematical degeneracy) Degenerate boundary (No subdomain and no hypersingularity) Degenerate scale True and spurious eigensolution (interior prob) Fictitious frequency (exterior acoustics)
Conclusions
Outline
3
Overview of numerical methods
Finite Difference M ethod Finite Element M ethod Boundary Element M ethod
M esh M ethods M eshless M ethods
Numerical M ethods
PDE- variational IEDE
Domain
BoundaryMFSTrefftz method MLS EFG
開刀 把脈
針灸
( 中醫式的工程分析法 )
4
BEM
USA China UK Germany France India Italy Iran Japan South Korea (Taiwan No11)
Dual BEM (Made in Taiwan)
UK USA Taiwan China Germany France Japan Brazil Australia Singapore (No3)
(ISI information updated March 21 2008)
Top ten countries of BEM and dual BEM
5
FEM USA China Germany France UK Japan India Tai
wan Turkey Italy (No8)
Meshless methods China USA Singapore Germany UK Taiwan Japan
Portugal Slovakia Australia (No6) FDM China USA Japan India France Taiwan Canada UK Italy South Korea (No6) (ISI information updated March 21 2008)
Top ten countries of FEM FDM and Meshless methods
6
BEM Zhang C (Germany) Sapountzakis E J (Greece) Sladek J and Sladek V (Slovakia twin) Chen J T (Taiwan Ocean Univ) 119 SCI papers gt 545 citing Mukherjee S (USA) Tanaka M (Japan) Dual BEM (Made in Taiwan) Aliabadi M H (UK Imperial College London) Chen J T (Taiwan Ocean Univ) Chen K H(Taiwan Ilan Univ) Power H (UK Univ Nottingham) (ISI information updated March 21 2008)
Active scholars on BEM and dual BEM
7
USA 劉毅軍教授
NTOUMSV Taiwan 海洋大學 陳正宗終身特聘教授
北京清華大學工程力學系 -姚振漢教授
高海大造船系 -陳義麟博士
台大土木系 -楊德良終身特聘教授
宜蘭大學土木系陳桂鴻博士
北京清華姚振漢教授提供
Top 25 scholars on BEMBIEM since 2001
8
Number of Papers of FEM BEM and FDM
(Data form Prof Cheng A H D)
126
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
2
Overview of numerical methods ( 中醫式的工程分析法 ) Nonuniqueness problems - review
BEM failure (mathematical degeneracy) Degenerate boundary (No subdomain and no hypersingularity) Degenerate scale True and spurious eigensolution (interior prob) Fictitious frequency (exterior acoustics)
Conclusions
Outline
3
Overview of numerical methods
Finite Difference M ethod Finite Element M ethod Boundary Element M ethod
M esh M ethods M eshless M ethods
Numerical M ethods
PDE- variational IEDE
Domain
BoundaryMFSTrefftz method MLS EFG
開刀 把脈
針灸
( 中醫式的工程分析法 )
4
BEM
USA China UK Germany France India Italy Iran Japan South Korea (Taiwan No11)
Dual BEM (Made in Taiwan)
UK USA Taiwan China Germany France Japan Brazil Australia Singapore (No3)
(ISI information updated March 21 2008)
Top ten countries of BEM and dual BEM
5
FEM USA China Germany France UK Japan India Tai
wan Turkey Italy (No8)
Meshless methods China USA Singapore Germany UK Taiwan Japan
Portugal Slovakia Australia (No6) FDM China USA Japan India France Taiwan Canada UK Italy South Korea (No6) (ISI information updated March 21 2008)
Top ten countries of FEM FDM and Meshless methods
6
BEM Zhang C (Germany) Sapountzakis E J (Greece) Sladek J and Sladek V (Slovakia twin) Chen J T (Taiwan Ocean Univ) 119 SCI papers gt 545 citing Mukherjee S (USA) Tanaka M (Japan) Dual BEM (Made in Taiwan) Aliabadi M H (UK Imperial College London) Chen J T (Taiwan Ocean Univ) Chen K H(Taiwan Ilan Univ) Power H (UK Univ Nottingham) (ISI information updated March 21 2008)
Active scholars on BEM and dual BEM
7
USA 劉毅軍教授
NTOUMSV Taiwan 海洋大學 陳正宗終身特聘教授
北京清華大學工程力學系 -姚振漢教授
高海大造船系 -陳義麟博士
台大土木系 -楊德良終身特聘教授
宜蘭大學土木系陳桂鴻博士
北京清華姚振漢教授提供
Top 25 scholars on BEMBIEM since 2001
8
Number of Papers of FEM BEM and FDM
(Data form Prof Cheng A H D)
126
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
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1994
1995
1996
1997
1998
1999
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2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
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1996
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2004
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Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
3
Overview of numerical methods
Finite Difference M ethod Finite Element M ethod Boundary Element M ethod
M esh M ethods M eshless M ethods
Numerical M ethods
PDE- variational IEDE
Domain
BoundaryMFSTrefftz method MLS EFG
開刀 把脈
針灸
( 中醫式的工程分析法 )
4
BEM
USA China UK Germany France India Italy Iran Japan South Korea (Taiwan No11)
Dual BEM (Made in Taiwan)
UK USA Taiwan China Germany France Japan Brazil Australia Singapore (No3)
(ISI information updated March 21 2008)
Top ten countries of BEM and dual BEM
5
FEM USA China Germany France UK Japan India Tai
wan Turkey Italy (No8)
Meshless methods China USA Singapore Germany UK Taiwan Japan
Portugal Slovakia Australia (No6) FDM China USA Japan India France Taiwan Canada UK Italy South Korea (No6) (ISI information updated March 21 2008)
Top ten countries of FEM FDM and Meshless methods
6
BEM Zhang C (Germany) Sapountzakis E J (Greece) Sladek J and Sladek V (Slovakia twin) Chen J T (Taiwan Ocean Univ) 119 SCI papers gt 545 citing Mukherjee S (USA) Tanaka M (Japan) Dual BEM (Made in Taiwan) Aliabadi M H (UK Imperial College London) Chen J T (Taiwan Ocean Univ) Chen K H(Taiwan Ilan Univ) Power H (UK Univ Nottingham) (ISI information updated March 21 2008)
Active scholars on BEM and dual BEM
7
USA 劉毅軍教授
NTOUMSV Taiwan 海洋大學 陳正宗終身特聘教授
北京清華大學工程力學系 -姚振漢教授
高海大造船系 -陳義麟博士
台大土木系 -楊德良終身特聘教授
宜蘭大學土木系陳桂鴻博士
北京清華姚振漢教授提供
Top 25 scholars on BEMBIEM since 2001
8
Number of Papers of FEM BEM and FDM
(Data form Prof Cheng A H D)
126
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
4
BEM
USA China UK Germany France India Italy Iran Japan South Korea (Taiwan No11)
Dual BEM (Made in Taiwan)
UK USA Taiwan China Germany France Japan Brazil Australia Singapore (No3)
(ISI information updated March 21 2008)
Top ten countries of BEM and dual BEM
5
FEM USA China Germany France UK Japan India Tai
wan Turkey Italy (No8)
Meshless methods China USA Singapore Germany UK Taiwan Japan
Portugal Slovakia Australia (No6) FDM China USA Japan India France Taiwan Canada UK Italy South Korea (No6) (ISI information updated March 21 2008)
Top ten countries of FEM FDM and Meshless methods
6
BEM Zhang C (Germany) Sapountzakis E J (Greece) Sladek J and Sladek V (Slovakia twin) Chen J T (Taiwan Ocean Univ) 119 SCI papers gt 545 citing Mukherjee S (USA) Tanaka M (Japan) Dual BEM (Made in Taiwan) Aliabadi M H (UK Imperial College London) Chen J T (Taiwan Ocean Univ) Chen K H(Taiwan Ilan Univ) Power H (UK Univ Nottingham) (ISI information updated March 21 2008)
Active scholars on BEM and dual BEM
7
USA 劉毅軍教授
NTOUMSV Taiwan 海洋大學 陳正宗終身特聘教授
北京清華大學工程力學系 -姚振漢教授
高海大造船系 -陳義麟博士
台大土木系 -楊德良終身特聘教授
宜蘭大學土木系陳桂鴻博士
北京清華姚振漢教授提供
Top 25 scholars on BEMBIEM since 2001
8
Number of Papers of FEM BEM and FDM
(Data form Prof Cheng A H D)
126
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
5
FEM USA China Germany France UK Japan India Tai
wan Turkey Italy (No8)
Meshless methods China USA Singapore Germany UK Taiwan Japan
Portugal Slovakia Australia (No6) FDM China USA Japan India France Taiwan Canada UK Italy South Korea (No6) (ISI information updated March 21 2008)
Top ten countries of FEM FDM and Meshless methods
6
BEM Zhang C (Germany) Sapountzakis E J (Greece) Sladek J and Sladek V (Slovakia twin) Chen J T (Taiwan Ocean Univ) 119 SCI papers gt 545 citing Mukherjee S (USA) Tanaka M (Japan) Dual BEM (Made in Taiwan) Aliabadi M H (UK Imperial College London) Chen J T (Taiwan Ocean Univ) Chen K H(Taiwan Ilan Univ) Power H (UK Univ Nottingham) (ISI information updated March 21 2008)
Active scholars on BEM and dual BEM
7
USA 劉毅軍教授
NTOUMSV Taiwan 海洋大學 陳正宗終身特聘教授
北京清華大學工程力學系 -姚振漢教授
高海大造船系 -陳義麟博士
台大土木系 -楊德良終身特聘教授
宜蘭大學土木系陳桂鴻博士
北京清華姚振漢教授提供
Top 25 scholars on BEMBIEM since 2001
8
Number of Papers of FEM BEM and FDM
(Data form Prof Cheng A H D)
126
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
6
BEM Zhang C (Germany) Sapountzakis E J (Greece) Sladek J and Sladek V (Slovakia twin) Chen J T (Taiwan Ocean Univ) 119 SCI papers gt 545 citing Mukherjee S (USA) Tanaka M (Japan) Dual BEM (Made in Taiwan) Aliabadi M H (UK Imperial College London) Chen J T (Taiwan Ocean Univ) Chen K H(Taiwan Ilan Univ) Power H (UK Univ Nottingham) (ISI information updated March 21 2008)
Active scholars on BEM and dual BEM
7
USA 劉毅軍教授
NTOUMSV Taiwan 海洋大學 陳正宗終身特聘教授
北京清華大學工程力學系 -姚振漢教授
高海大造船系 -陳義麟博士
台大土木系 -楊德良終身特聘教授
宜蘭大學土木系陳桂鴻博士
北京清華姚振漢教授提供
Top 25 scholars on BEMBIEM since 2001
8
Number of Papers of FEM BEM and FDM
(Data form Prof Cheng A H D)
126
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
7
USA 劉毅軍教授
NTOUMSV Taiwan 海洋大學 陳正宗終身特聘教授
北京清華大學工程力學系 -姚振漢教授
高海大造船系 -陳義麟博士
台大土木系 -楊德良終身特聘教授
宜蘭大學土木系陳桂鴻博士
北京清華姚振漢教授提供
Top 25 scholars on BEMBIEM since 2001
8
Number of Papers of FEM BEM and FDM
(Data form Prof Cheng A H D)
126
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
8
Number of Papers of FEM BEM and FDM
(Data form Prof Cheng A H D)
126
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
9
有限元素成長史
0
1000
2000
3000
4000
5000
6000
1974
1975
1976
1977
1978
1979
1980
1981
1982
1983
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1985
1986
1987
1988
1989
1990
1991
1992
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
FE
M
邊界元素成長史
0
200
400
600
800
1000
1200
1400
1600
1975
1976
1977
1978
1979
1980
1981
1982
1983
1984
1985
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1988
1989
1990
1991
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1995
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1997
1998
1999
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2001
2002
2003
2004
2005
2006
2007
Year
Num
ber
of p
aper
s on
BE
M
March 21 2008
Cauchy kernel
Hadamard kernelBEM (no crack)
Dual BEM (crack)Small scale
Large scale
Early
Late
351
FMM(degenerate kernel)
NTOUMSV
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
10
Advantages of BEM
Discretization dimension reduction Infinite domain (half plane) Interaction problem Local concentration
Disadvantages of BEM Integral equations with singularity Full matrix (nonsymmetric)
北京清華
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
11
BEM and FEM
(1) BEM and meshless methods can be seen as a supplement of FEM
(2) BEM utilizes the discretization concept of FEM as well as the limitation Whether the supplement is needed or not depends on its absolutely superio
r area than FEM
C rack amp large scale problems
NTUCE
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
12
Disclaimer (commercial code)
The concepts methods and examples using
our software are for illustrative and educational purposes only Our cooperation assumes no liability or responsibility to any person or company for direct or indirect damages resulting from the use of any information contained here
inherent weakness
misinterpretation User 當自強
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
13
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
14
Nonuniqueness in numerical methods Nonlinear equation (spurious root) Finite difference method
spurious eigenvalue Finite element method amp meshless methods
spurious mode Boundary element method
spurious eigenvalues
fictitious frequency Boundary element method
degenerate scale
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
15
Nonuniqueness in solving nonlinear Eq Nonlinear equation (spurious root)
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
16
Why spurious solution occurs
2 2
2 2
2
6 2 1
( 6 2 ) (1 )
( 3 5) (2 )
9 34 25 0
( 1)(9 25) 0
251
9
x x
x x
x x
x x
x x
x or x
1 1 6 2 1 1 1 ( )
25 25 252 6 2 1 1 ( )
9 9 9
Ox
x
K
spu
tru
riou
e
s
國中數學經驗
兩邊平方後整理
再ㄧ次兩邊平方後整理
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
17
Nonuniqueness in FDM for ODE Finite difference method
solve first-order ODE
using Euler scheme (Greenberg 1998)
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
18
假根浮根溢根(Spurious Eigenvalue) 用中間差分的方法來逼近處理
2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
n nn
n n n
y x y xy x
hhy x y x y x
y
y y hy h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
THORN - = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc
0y hcent
X
y(x)
x0 x5 x1 x2 x3 x4
0 h 2h 3h 4h 5h
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
19
假根浮根溢根(Spurious Eigenvalue)
h=005 2 0 1y x y x y( ) ( ) ( )cent =- =
1 1
1 1
0
1 0 0
24
1
1 2
0 05
n nn
n n n
solution of FDM
y x y xy x
hhy x y x y x
y
y y hy h
h
( ) ( )( )
( ) ( ) ( )
+ -
+ -
-cent =
- = -
igrave =iumliumliacuteiuml cent= + = -iumlicirc=
2xexact solution e -
1 2 3 4
-75
-5
-25
25
5
75
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
20
Nonuniqueness in FDM for eigenproblems Finite difference method
solve eigenproblem (S Zhao 2007)
spectral type
nonspectral type
rod beam and membrane
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
21
Nonuniqueness in FEM and meshless method
Hour glass mode (solid mechanics)
shear locking
incompressible (solid propellant grain) Solid mechanics
incompressible flow Fluid mechanics
reduced integration
Edge element-divergence free (electromagnetics)
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
22
Solid mechanics (spurious mode)
UCLA J S Chen 2008
Physics Mathematics
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
23
Nonuniqueness in BEM for degenerate boundary BEM with degenerate boundary
1 2
3
4
56
7
8
Cutoff wall crack Thin airfoil
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
24
What Is Boundary Element Method
NTUCE
1 2
3
45
6
1 2
geometry nodethe Nth constantor linear element
N
西醫 郎中
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
25
Dual BEM
Why hypersingular BIE is required
(Two ways since 1986)
NTUCE
1 2
3
4
56
7
8
1 2
3
4
56
7
8
910
Artifical boundary introduced
BEM
Multi-domain
Dual integral equations needed
Dual BEM
Single-domain
Degenerate boundary
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
26
Some researchers on Dual BEM (1012)Chen (1986) 544 citings in total
Hong and Chen (1988 ) 78 citings ASCE EM
Portela and Aliabadi (1992) 212 citings IJNME
Mi and Aliabadi (1994)
Wen and Aliabadi (1995)
Chen and Chen (1995) 新竹清華 Yao (2005) 北京清華 黎在良等 --- 斷裂力學邊界數值方法 (1996) 周慎杰 (1999)
Chen and Hong (1999) 88 citings ASME AMR
Niu and Wang (2001)
Kuhn G Wrobel L C Mukherjee S Tuhkuri J Gray L J
Yu D H Zhu J L Chen Y Z Tan R J hellip
NTUCE
cite
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
27
Dual Integral Equations by Hong and Chen(1984-1986)
NTUCE
Singular integral equation Hypersingular integral equation
Cauchy principal value Hadamard principal value
(Mangler principal value)Boundary element method Dual boundary element method
normal
boundarydegenerate
boundary
1969 1986 2008
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
28
Degenerate boundary
geometry node
the Nth constantor linear element
un0
un0
un0
u 1 u 1(00)
(-105)
(-1-05)
(105)
(1-05)
1 2
3
4
56
7
8 [ ] [ ] U t T u
[ ] [ ] L t M u
N
1693-0335-019001904450703044503350
0334-1693-281028100450471034700390
00630638-193119316380063008100810
00630638-193119316380063008100810
04710045-281028106931335003903470
07030445019001903350693133504450
04710347054005400390335069310450
0335-0039054005403470471004506931
][
U
-1107464046402190490021901071
1107-7850785400000588051909270
088813263261888092709270
088813263261888092709270
0588000078507850107192705190
0490021946404640107110712190
0588051932103210927010710000
1107092732103210519058800000
][
T
5(+) 6(+) 5(+) 6(-)
5(+)6(+)
5(+)6(+)
n s( )
0805464046406120490061208050
0805347034700000184051909270
088814174171888051105110
0888-1417-4171888051105110
0184000034703470805092705190
0490061246404640805080506120
0184051945804580927080500000
0805092745804580519018400000
][
L
00041600-400040002820235028206001
1600-0004000100013331205006208000
0715-3765-000800087653715085308530
07153765000800087653715085308530
0205-1333-000100010004600180000610
0236-0282-400040006001000460012820
0205-0061-600060008000600100043331
1600-0800-600060000610205033310004
][
M
5(+) 6(+)5(+) 6(-)
5(+)6(-)
5(+) 6(-)
n x( ) n x( )
n s( )
dependency
Nonuniqueness
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
29
The number of constraint equation is not enough to
determine coefficients of p and q
Another constraint equation is obtained by differential operator
axwhenqpaaf
qpxxQaxxf
)(
)()()( 2
axwhenpaf
pxQaxxQaxxf
)(
)()()()(2)( 2
How to get additional constraints
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
30
Original data from Prof Liu Y J
(1984)
crack
BEMCauchy kernel
singular
DBEMHadamard
kernelhypersingular
FMM
Large scaleDegenerate kernel
Desktop computer fauilure
(2000)Integral equation
1888
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
31
Successful experiences since 1986 (degenerate boundary)
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
32
Solid rocket motor (Army 工蜂火箭 )
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
33
X-ray detection ( 三溫暖測試 )
Crack initiation crack growth
Stress reliever
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
34
FEM simulation
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
35
Stress analysis
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
36
BEM simulation (Army)
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
37
Shong-Fon II missile (Navy)
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
38
V-band structure (Tien-Gen missile)
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
39
FEM simulation
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
40
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
41
Seepage flow (Laplace equation)
Sheet pileCutoff wall
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
42
Meshes of FEM and BEM
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
43
FEM (iteration No49) BEM(iteration No13)
Initial guessInitial guess
After iteration After iteration
Remesh areaRemesh line
Free surface seepage flow using hypersingular formulation
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
44
Incomplete partition in room acoustics(Helmholtz equation)
U T L Mm ode 1
m ode 2
m ode 3
000 0 05 0 10 0 15 0 200 00
0 05
0 10
0 00 0 05 0 10 0 15 0 200 00
0 05
0 10
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
000 005 010 015 020000
005
010
005 010 015 020
005
5876 H z 5872 H z
14437 H z 14443 H z
15173 H z 15162 H z
b
a
e
c
2 2 0u k u t0
t=0
t=0
t=0
t=0
t=0
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
45
Water wave problem with breakwaterWater wave problem with breakwater(modified Helmholtz equation)(modified Helmholtz equation)
Free water surface S
x
Top view
O
y
zO
xz
S
breakwater
breakwater
oblique incident water wave 0)~()~( 22 xuxu
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
46
Reflection and Transmission
000 040 080 120 160 200
kd
000
040
080
120
lRl a
nd lT
l
k h = 5D e ep w a te r th eo ry (U rse ll 1 9 4 6 )M u lti-d o m a in B E M (L iu e t a l 1 9 8 2 )U T m e th o d o f D B E M (C o m b in e d L M 3 2 0 e le m en ts)L M m e th o d o f D B E M (C o m b in e d U T 3 2 0 e le m en ts)
R
T
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
47
Cracked torsion bar
T
da
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
48
IEEE J MEMS
Comb drive
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
49
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
50
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
51
Is it possible
No hypersingularity
No subdomain
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
52
Dual BEM
Degenerate boundary problems
u=0r=1
0)()( 22 xukC
C
u=0r=1
0)()( 22 xukC C
CC
u=0r=1
0)()( 22 xukC
C
interface
Subdomain 1
Subdomain 2
Subdomain 1
Subdomain 2
1cu
1cu
1fu
1fu
2fu
2fu
2ft
1ft
2ft
1ft
2cu
2cu
1cu
1cu
C
C
C
C
Multi-domain BEM
][
][][
tLuM
tUuT
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
53
Rank deficiency due to degenerate boundary and rigid body mode (SVD)
PhysicsMathematics 2d
SC
C
-12 -8 -4 0 4 8 12
-12
-8
-4
0
4
8
12
Left unitary matrix Right unitary matrix
U
Spurious True
L
T
M
Rigid body mode
left unitary vector UK-1( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-1( )
-07
-06
-05
-04
-03
-02
-01
0
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vector MK-1( )
000501
01502
02503
03504
045
1 2 3 4 5 6 7 8 9 10
1數列
right unitary vecto TK-1( )
-04
-035
-03
-025
-02
-015
-01
-005
0
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector UK-2( )
-08
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
left unitary vector LK-2( )
-06
-04
-02
0
02
04
06
08
1 2 3 4 5 6 7 8 9 10
1數列
1 spurious mode(fictitious mode)
(mathematics)
1 true mode rigid body mode
(physics)
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
54
SVD Technique (Google searching)
nnnmmmnm VUC
][][][][
[C] SVD decomposition
[U] and [V left and right unitary vectors
nm
nm
n
00
00
0
0
][ 1
11 nn
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
55
Physical meaning of SVD
1 2 3 1 2 3 =[ ] =[ ]TF 變形前變形後
假根 真根Chen et al 2002 Int J Comp Numer Anal Appl
先拉再轉 先轉再拉
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
56
Conventional BEM in conjunction with SVD
Singular Value DecompositionH
PPPMMMPMU ][][][][
Rank deficiency originates from two sources
(1) Degenerate boundary
(2) Nontrivial eigensolution
Nd=5 Nd=5Nd=4
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
57
0 2 4 6 8
k
0001
001
01
1
N d + 1
0 2 4 6 8
k
1e-020
1e-019
1e-018
1e-017
1e-016
1e-015
1e-014
d e t [ U ( k ) ]
0 2 4 6 8
k
1e-038
1e-037
1e-036
1e-035
1e-034
d e t [ K U
L ]
Dual BEM
UT BEM + SVD
(Present method)
versus k1dN
Determinant versus k
Determinant versus k
Sub domain
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
58k=314 k=382
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=448
UT BEM+SVD
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
-0 8 -0 6 -0 4 -0 2 0 02 04 06 08
-0 8
-0 6
-0 4
-0 2
0
02
04
06
08
k=309
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=384
-08 -06 -04 -02 0 02 04 06 08
-08
-06
-04
-02
0
02
04
06
08
k=450
FEM (ABAQUS)
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
59
Nonuniqueness in BEM for exterior acoustics
BEM for exterior acoustics
Numerical and physical resonance
a
m
k
e i t
incident wave
e i t e i t
radiation
Physical resonance Numerical resonance
if ufinite
( )
2 2
if u finite lim00
m
k
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
60
Radiation and scattering problems
Nonuniform radiaton scattering
1)( au0)( au
Drruk )( 0)()( 22
32
5
Drruk )( 0)()( 22
2
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
61
Errorestimator
Error estimator
SolutionSolution
Strategy of adaptive BEM
Miller ampBurton
SingularEquation
ut Mk
iTL
k
iU
~~
][][
tu UTUT~~
][][
HypersingularEquation
tu LMLM~~
][][
ut ut
21
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
62
BEM FEM
Adaptive Mesh
- 1 - 1 0 1 1
- 1
- 1
0
1
1
5
DtN interface
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
63
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
-150 -100 -050 000 050 100 150
-150
-100
-050
000
050
100
150
Numerical solution BEM Numerical solution FEM
64 ELEMENTS 2791 ELEMENTS
Nonuniform radiation Dirichlet problem
2ka
9
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
64
Numerical phenomena(Fictitious frequency)
0 2 4 6 8
-2
-1
0
1
2UT method
LM method
Burton amp Miller method
t(a0)
1)( au0)( au
Drruk )( 0)()( 22
9
1)( au0)( au
Drruk )( 0)()( 22
9
A story of PhD students
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
65
Nonuniqueness in BEM for degenerate scale BEM with degenerate scale Gamma contour Critical value Logarithmic capacity Solvability of integral equations Invertibility of integral operator
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
66
Numerical phenomena(Degenerate scale)
Error ()of
torsionalrigidity
a
0
5
125
da
Previous approach Try and error on aPresent approach Only one trial
T
da
Commercial ode output
Stokes Flowbiharmonic
TorsionLaplace
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
67
Nonuniqueness in BEM for multiply connected domain problem
Spurious eigensolution
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
68
Numerical phenomena (2-D)(Spurious eigensolution)
0 1 2 3 4 5 6 7 8 9 10 11 12fre q u e n cy p a ra m e te r
1E-080
1E-060
1E-040
1E-020
de
t|SM
|
C -C annular p la teu com plex-vauled form ulation
Tlt9447gt
T T rue e igenvalues
Tlt10370gt
Tlt10940gt
Tlt9499gt
Tlt9660gt
Tlt9945gt
Slt9222gt
Slt6392gt
Slt11810gt
S Spurious e igenvalues
ma 1
mb 50
1B
2B
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
69
Numerical phenomena (3-D)(Spurious eigensolution)
x
y
z
a
05a
04a
BIEM Experiment Inner (spurious) ABAQUS
1110 113 85357
2012 204 18649 ( 2 )
2771 279 20985
3649 364 24775 ( 2 )
4385 441 4263 2745
6421 640 6100 30505 ( 2 )
7826 784 7820 3333
8492 854 8525 35002
9126 907 37471 ( 2 )
9313 933 3993 ( 2 )
9961 990 helliphelliphellip
10406 1033 helliphelliphellip
呂學育博士林羿州Fillipi JSV
Spuriouseigenvalue
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
70
TreatmentsSVD updating term
Burton amp Miller method
CHIEF method
NN
cc
cc
SM
SMC
8162
1
cccc SMiSM21
NNN cCCUCUC
CCUCUC
UU
UU
UU
UU
C
8)4(2
2121
2121
22212221
12111211
22212221
12111211
][
Mathematical analysis and numerical study for free vibration of plate using BEM-70
a
b
1B
2B
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
71
SVD structure for four influence matrices
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
72
SVD updating technique ( 去蕪 [ ] 存精 ( ) 術 )
U TL M
11
0 ULUT
11
0 TMUT
11
0 ULLM
11
0 TMLM
1 spurious mode fictitious mode (mathematics)
1 true mode rigid body mode (physics)
The same
The same
The same The same[ ]()
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
73
BEM trap Why engineers should learn
mathematics Well-posed Existence Unique
Mathematics versus Computation
equivalent 馮康 定理
Some examples
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
74
馮康 定理 同一個物理或工程問題可以有各種不同
的數學模式來模擬 這些數學模式在物理上是等效的 (Equivale
nt) 但在離散後數值的實踐 (Implementation) 就不見得等效
唯有在不同的數值方法中儘量保有問題的基本特徵方是做計算數學與計算力學的最高指導原則 10524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425105242510524251052425
104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965 104996510499651049965104996510499651049965104996510499651049965104996510499651049965104996510499651049965
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
75
Conclusions
bull Review of numerical methods ( 中醫式的工程分析法 )
bull Review of nonuniqueness problems in numerical method
s
bull Successful experiences in the engineering applications wi
th degenerate boundaries were demonstrated
bull Nonuniquness due to degenerate boundary degenerate s
cale spurious eigenvalue fictitious frequency is shown
bull SVD structures for the nonuniqueness are examined
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
76
Acknowledgementbull 台大土木系 洪宏基 終身特聘教授bull 中山科學院 王政盛博士bull 高海大造船系 陳義麟博士
bull 宜大土木系 陳桂鴻 博士 bull 中華技術學院機械系 李為民 博士bull 中華技術學院機械系 呂學育 博士bull 中山科學院 全湘偉博士bull NTOUMSV group members
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79
77
The End
Thanks for your kind attention
78
歡迎參觀海洋大學力學聲響振動實驗室烘焙雞及捎來伊妹兒
httpindntouedutw~msvlabhttp140121146149
E-mail jtchenmailntouedutw
79