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8/10/2019 Pqe Vibration 09 Solution 1
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COLLEGE OF ENGINEERING
MECHANICAL ENGINEERING
Ph.D. Preliminary Qualifying Examination
Signature PageVibration Examination (Modify)
January 26 2!!" (Monday)##Modify"$!! am % &2$!! noon
Room 2145 Engineering Building
'or identifiation uro*e* lea*e fill out the follo+ing information in in,. -e *ureto rint and *ign your name. hi* o/er age i* for attendane uro*e* only and+ill be *earated from the re*t of the exam before the exam i* graded. 0rite your*tudent number on all exam age*. Do 1 +rite your name on any of the otherexam age* be*ide* the o/er age.
Name (print in INK)
Signature (in INK)
Student Number (in INK)
Do all your +or, on ro/ided *heet* of aer. 3f you need extra *heet* lea*ere4ue*t them from rotor. 0hen you are fini*hed +ith the te*t return the examlu* any additional *heet* to the rotor.
8/10/2019 Pqe Vibration 09 Solution 1
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COLLEGE OF ENGINEERING
MECHANICAL ENGINEERING
Ph.D. Preliminary Qualifying Examination
5o/er Page
"$!! am % &2$!! noonRoom 2145 Engineering Building
E1E789 31S7:531S$
hi* examination ontain* fi/e roblem*. ;ou are re4uired to *elet and *ol/e four of the fi/e roblem*. 5learly indiate the roblem* you +i*h to be graded. 3f youattemt *ol/ing all of them +ithout indiating +hih four of your hoie the four
roblem* +ith the +or*t grade* +ill be on*idered. 1ote that Problem number 5 is mandatory.
Do all your +or, on the ro/ided *heet* of aer. 3f you need extra *heet* lea*ere4ue*t them from the rotor. 0hen you are fini*hed +ith the te*t return theexam lu* any additional *heet* to the rotor.
8/10/2019 Pqe Vibration 09 Solution 1
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Mehanial Engineering Ph.D. Preliminary Qualifying ExaminationVibration % January 26 2!!"
You are required to wor !our o! t"e !i#e problem$% one o! w"i&" i* Problem 1o. <' learlindi&ate w"i&" problem$ ou are &"oo$ing' S"ow all wor on t"e e*am $"eet$ pro#ided and write
our $tudent per$onal identi!i&ation (+I,) number on ea&" $"eet' ,o not write our name on an$"eet'
Your +I, number-............................
Que*tion =&
/ uni!orm bar o! lengt" L and weig"t W i$ $u$pended $mmetri&all b twoun$tre&"able $tring$ a$ $"own in t"e !igure' I! t"e bar i$ gi#en $mall initial rotation aboutt"e #erti&al a*i$%
a' ,raw t"e !ree bod diagram o! t"e bar during it$ !ree o$&illation' b' 0rite down t"e equation o! motion !or $mall angular o$&illation about a*i$ '&' ,etermine t"e period o! t"e !ree o$&illation o! t"e bar'
O
O L
a
h
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You are required to wor !our o! t"e !i#e problem$' learl indi&ate w"i&" problem$ ou are&"oo$ing' S"ow all wor on t"e e*am $"eet$ pro#ided and write our $tudent per$onal
identi!i&ation (+I,) number on ea&" $"eet' ,o not write our name on an $"eet'
Your +I, number-............................
Que*tion =23"e $$tem $"own in t"e !igure i$ in it$ $tati& equilibrium po$ition (SE+)' It &on$i$t$ o! auni!orm rod o! ma$$ m and lengt" L and i$ $upported b $pring o! $ti!!ne$$ k andda$"pot o! &oe!!i&ient c '
a' ,raw t"e !ree bod diagram o! ea&" $$tem a$ it o$&illate$ about t"e SE+' b' ,eri#e t"e equation o! motion o! ea&" $$tem u$ing Newton$ $e&ond law'
&' ,etermine t"e undamped natural !requen&'d' ,etermine t"e damping ratio% t"e &riti&al damping &oe!!i&ient% and t"e dampednatural !requen&'
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You are required to wor !our o! t"e !i#e problem$' learl indi&ate w"i&" problem$ ou are&"oo$ing' S"ow all wor on t"e e*am $"eet$ pro#ided and write our $tudent per$onalidenti!i&ation (+I,) number on ea&" $"eet' ,o not write our name on an $"eet'
Your +I, number-............................
Que*tion =>3"e $$tem $"own &on$i$t$ o! a &linder o! ma$$ m wit" a pi$ton% w"i&" impart$re$i$tan&e proportional to t"e #elo&it o! a linear #i$&ou$ damping c % t"e &linder i$re$trained b a $pring o! $ti!!ne$$ k
(a) draw t"e !ree bod diagram o! t"e &linder%
(b) write down t"e equation o! motion u$ing Newton$ $e&ond law% and
(&) determine t"e re$pon$e amplitude and p"a$e angle u$ing 5omlex 8lgebra'
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You are required to wor !our o! t"e !i#e problem$' learl indi&ate w"i&" problem$ ou are&"oo$ing' S"ow all wor on t"e e*am $"eet$ pro#ided and write our $tudent per$onalidenti!i&ation (+I,) number on ea&" $"eet' ,o not write our name on an $"eet'
Your +I, number-............................
Que*tion =?
3"e $$tem $"own below &on$i$t$ o! two rotor$ &oupled b a di$&ontinuou$ $"a!t o!
modulu$ o! rigidit i$ 211'5 16 7 7G lb in rad = × -
• ,raw t"e !reebod diagram o! ea&" rotor%
• ,eri#e t"e equation$ o! motion%
• ,etermine t"e natural !requen&ie$ o! !ree tor$ional o$&illation$ and pro#ide t"e
p"$i&al meaning o! ea&" #alue%
• ,raw t"e normal mode $"ape and e#aluate t"e #alue o! t"e twi$t at t"e 8un&tion o!
t"e two $"a!t$% i'e' 17nθ θ or 27nθ θ
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M81D87; P7-9EM (E9ERYNE IS RE:;IRE, 3 S<9E 3=IS +RB<E>) Your +I, number-............................
Que*tion =<
on$ider a rigid bod o! ma$$ m and ma$$ moment o! inertia J c wit" re$pe&t to &enter o! gra#itC g ' Suppo$e t"at t"e bod i$ $upported b two $pring$ o! $ti!!ne$$ k t"at are atta&"ed at di$tan&e$2l and l wit" re$pe&t to t"e &enter o! gra#it C g a$ $"own in ?igure 5a' <et m @ 16 g% J c @ 5 gm2
k @ 166 N7m% and l @ 1 m'
+art I-
(a) ,eri#e t"e equation$ o! motion !or t"i$ bod u$ing &oordinate$ x and θ '
(b) ,etermine t"e natural !requen&ie$ o! t"e $$tem'
(&) ,raw t"e natural mode $"ape$ o! t"e $$tem'
(5a) (5b)
Ne*t% &on$ider t"e $ame rigid bod a$ $"own in ?igure 5b'
+art II-
(d) ,eri#e t"e equation$ o! motion !or t"i$ bod u$ing &oordinate$ x1 and x2'
(e) ,etermine t"e natural !requen&ie$ o! t"e $$tem'
(!) ,raw t"e natural mode $"ape$ o! t"e $$tem'
+art III-(g) State i! t"ere are di!!eren&e$ in t"e equation$ o! motion% natural !requen&ie$ and mode
$"ape$ obtained in ea&" &a$e and e*plain w"'
(") 0"at are t"e &oupling$ in equation$ o! motion% re$pe&ti#el% in t"e$e two &a$e$A
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+roblem 1
/ uni!orm bar o! lengt" L and weig"t W i$ $u$pended$mmetri&all b two $tring$ a$ $"own in t"e !igure' I! t"e bar i$ gi#en $mall initial rotation about t"e #erti&al a*i$%
d' ,raw t"e ?B, o! t"e bar during it$ !ree o$&illation'e' 0rite down t"e equation o! motion !or $mall angular
o$&illation about a*i$ '!' ,etermine t"e period o! t"e !ree o$&illation o! t"e bar'
?igure 5'Solution-
'-D
?rom t"e $tati& equilibrium po$ition we write
23 mg=
(1);nder !ree #ibration o! t"e bar and in an arbitrar po$ition θ % t"e bar will be rai$ed up
$lig"tl% and will be di$pla&ed b a di$tan&e ( 7 2)a θ !rom t"e it$ $u$pended $tring' 3"e
$tring al$o be tilted b an angle ϕ !rom t"e #erti&al $u&" t"at% ( 7 2) "a θ = ϕ ' 3"i$
geometri& relation gi#e$ ( 7 2")aϕ = θ '
Now writing t"e equation o! motion b taing moment$ about a*i$ % gi#e$
6I 2(3$in )( 7 2) 3 3
2"
aa a a
θ = − ϕ ≈ − ϕ = − θ ÷
&&
(2);$ing equation (1)% equation (2) tae$ t"e !orm
2
6 n
6
mg mgI 6 6 6
4" 4I "
2 2a aθ + θ = → θ + θ = → θ + ω θ =&& && &&
()
O
O L
a
h
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w"eren 22
6
mg mg g
4I " "<<4 m "
12
2 2 2a a aω = = =
÷
(4)
+roblem 2
'-D
(b) ?rom t"e !reebod diagram% we write t"e equation o! motion !rom t"e $tati&equilibrium po$ition u$ing Newton$ $e&ond law o! moment$ about t"e "inge a*i$
( ) ( )2
2 2
66
mL I cL L ka a cL kaθ θ θ θ θ θ = − − → + + =&& & && & (1)
(&) 3"e undamped natural !requen& i$ obtained b di#iding bot" $ide$ o! t"e equation o!
motion (1) b t"e &oe!!i&ient o! θ &% i'e'%
2 2
2 2 6
n
c ka ka a k
m mL mL L m
θ θ θ ω + + = → = =&& & (2)
(d) 3"e damping ratio i$ obtained b writing t"e equation o! motion in t"e !orm22 6
n nθ ζω θ ω θ + + =&& & ()
3"u$ we &an write km
2
2 2 2
n
n
c c c cL
m m a k kmam
L m
ζω ζ ω
= → = = = (4)
3"e &riti&al damping &oe!!i&ient i$ obtained !rom (4) a$
2
2 cr
cr
c cL kmac
c Lkmaζ = = → =
3"e damped natural !requen&% nd ω % i$ written in term$ o! t"e undamped natural
!requen&% nω % a$
2 2 2
2
2
C1 1 1
122 nd n
a k cL a k c L
L m L m kmakmaω ω ζ
= − = − = − ÷
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+roblem D
;$ing Newton$ $e&ond law and wit" t"e
"elp o! t"e ?B,% t"e equation o! motion i$
( )mx kx c y x= − + −&& & & (1)
Rearranging
mx cx kx cy+ + =&& & (1a)
But ( ) $in Im i t y t Y t Y e Ω= Ω = (2)
/l$o ( ) &o$ Im i t y t Y t i Y e Ω= Ω Ω = Ω& ()
Note t"at one &an write( ) ( ) ( ) ( )
7 2 72 be&au$e &o$ 7 2 $in 7 2
i ii e e i i
π π π π = = + =
3"u$ one &an write equation (1a) in t"e !orm
2Im Imi t
i t mx cx kx icY e cY eπ Ω + ÷Ω + + = Ω = Ω&& &
(4)
3"e re$pon$e mu$t o$&illate at t"e $ame !requen& o! t"e e*&itation in t"e $tead $tate atamplitude and p"a$e angle to be determined% t"u$ one &an write t"e re$pon$e in t"e !orm
( ) w"erei t i i t i x t X Ime X Ime X X Imeϕ ϕ Ω − Ω −= = = (5)
0e need t"e !ir$t and $e&ond time deri#ati#e$ o! ( ) x t % i'e'
2( ) % ( )i t i t x t i X Ime x t X ImeΩ Ω= Ω = −Ω& && ()
Sub$tituting e*pre$$ion$ (5) and () into equation (4)% gi#e$
2 22 2i t
i t i t i t
n n n X Ime i X Ime X Ime Y Ime
π
ζω ω ζω
Ω + ÷Ω Ω Ω + Ω + = Ω ()
an&eling out i t Ime Ω !rom bot" $ide$ o! equation () and rearranging% gi#e$
2 2 2 22 2 2 % w"erei i
n n n n X i X X Y Ime Y Y Y Ime
π π
ζω ω ζω ζω −Ω + Ω + = Ω = Ω = (F)
Rearranging
( )2 2
2
2
n
n n
X
Y i
ζω
ω ζω
Ω=
− Ω + Ω (C)
>ultipling and di#iding b t"e &on8ugate o! t"e denominator% gi#e$
( )( )( )
2 2
2 2 2 2
22
2 2
n nn
n n n n
i X
Y i i
ω ζω ζω
ω ζω ω ζω
− Ω − ΩΩ= ×
− Ω + Ω − Ω − Ω
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( ) ( )
( )2 2
2 22 2
22
2
n
n n
n n
iζω
ω ζω ω ζω
Ω = − Ω − Ω − Ω + Ω
(16)
,i#iding t"e numerator and denominator b2
nω % and $etting 7
nr ω = Ω % equation (16)
tae$ t"e !orm
( ) ( )( )2
2 22
21 2
1 2
X r r i r
Y r r
ζ ζ
ζ
= − −
− + (11)
>ultipling and di#iding ea&" e*pre$$ion b ( ) ( )2 22
1 2r r ζ − + gi#e$
( ) ( )
( ) ( )
( )
( ) ( ) ( ) ( )
2 22 2
2 2 2 22 2 22 2
2 1 2 1 2
1 21 2 1 2
r r r r X r i
Y r r r r r r
ζ ζ ζ
ζ ζ ζ
− + − = −
− + − + − +
(12)
0it" t"e "elp o! t"e $"own triangle equation (12)ma be written in t"e !orm
( ) ( )
[ ]2 22
2&o$ $in
1 2
X r i
Y r r
ζ ψ ψ
ζ
= −
− + (1)
E*pre$$ing X and Y in term$ o! t"eir original
,e!inition$ (5) and (F)% gi#e$
( ) ( )[ ]7 2 2 22
2
&o$ $in1 2
i
i
X Ime r
iY Imer r
ϕ
π
ζ
ψ ψ ζ
−
= −− +
( ) ( )[ ]
( ) ( )
72
2 22 22 2
2 2&o$ $in
1 2 1 2
i i
i X Ime r r i IM e
Y r r r r
ϕ π ψ ζ ζ
ψ ψ
ζ ζ
− −−= − =
− + − +% t"u$
( ) ( )
1
22 22
2 2% and 7 2 or 7 2 tan 72
11 2
r r X i i i
r r r
ζ ζ ϕ π ψ ϕ ψ π ϕ π
ζ
−= − − = − = − → = −−− +
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+roblem 4
In$ert a #irtual di$ at t"e $"a!t di$&ontinuit o! moment o! inertia 6n
J = % t"e
&orre$ponding twi$t angle i$ nθ ' 3"e equation$ o! motion o! t"e t"ree degree$ o! !reedom
are
1 1 1 1( )n J K θ θ θ = −&& % 1 1 2 2( ) ( ) 6n n n n J K K θ θ θ θ θ = − − + − =&& % 2 2 2 2( )n J K θ θ θ = − −&&
!rom t"e $e&ond equation we "a#e- 1
1 2 1 22 2 2
( ) 6'15 16 6'6C41 16 ( 6'5CC) 6'65C 16n n K K K K θ θ θ
θ θ θ + = + → × = × − + ×
3"u$2
6'621
1
nθ
θ = −
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+roblem 5Solution to +roblem 5-+art I-3"e equation$ o! motion &an be deri#ed a$ !ollow$-
∑ = xm F → ( ) ( )θ θ l xk l xk xm +−−−= 2
θ C C J M ∑ = → ( ) ( )θ θ θ l xkl l xkl J C +−−= 22
w"i&" lead$ to t"e !ollowing matri* equation$
=
−
−+
6
6
5
2
6
62
θ θ
x
kl kl
kl k x
J
m
C
(1)
/$$ume t X x ω $in= and t ω θ $inΘ= % and $ub$titute t"e a$$umed !orm $olution$ intoEq' (1)'
=
Θ
−−
−−
6
6
5
2
22
2 X
J kl kl
kl mk
C ω
ω % (2)
3"e natural !requen&ie$ &an be determined b $etting t"e determinant o! Eq' (2) to Gero
65
2det
22
2
=
−−−−
ω
ω
C J kl kl
kl mk % w"i&" ield$
( )( ) 652 22222 =−−− l k J kl mk
C ω ω ()
Equation () i$ t"e &"ara&teri$ti& equation o! t"e $$tem' Sub$titute J C @ 6'5ml 2 into ()
61F12 2242 =+− k mk m ω ω % (4)
3"ere!ore% t"e natural !requen&ie$ are
( ) 2'42B51 =−= mk ω (rad7$e&) and ( ) 1'162B5
2 =+= mk ω (rad7$e&)' (5)
Sub$tituting t"e natural !requen&ie$ into t"e "omogeneou$ part o! Eq' (2) gi#e$ t"enatural mode$ o! t"e $$tem-
( )
( ) 1'42B4
1
2 2
1
1
1
=+−
=−
=Θ ω mk
k
l
X and
( )
( ) 1'62B4
1
2 2
2
2
2
−=−−
=−
=Θ ω mk
k
l
X ' ()
1$t mode $"ape 2nd mode $"ape
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+art II-
3"e equation$ o! motion &an be deri#ed a$ !ollow$-
∑ = xm F → 2121
B
2
Bkxkx
x xm −−=
+
θ C C
J M ∑ = → 2112 2
BBklxklx
l
x
l
x J C
−=
−
w"i&" lead$ to t"e !ollowing matri* equation$% a!ter $ub$tituting J C @ 6'5ml 2
=
−
+
− 6
6
12
BB2
2
1
2
1
x
x
k k
k k
x
x
mm
mm
()
/$$ume t X x ω $in11
= and t X x ω $in22 = % and $ub$titute t"e a$$umed !orm $olution$
into Eq' (1)'
=
−+−
−−
6
6
12
2BB
2
1
22
22
X
X
mk mk
mk mk
ω ω
ω ω
% (F)
3"e natural !requen&ie$ &an be determined b $etting t"e determinant o! Eq' (F) to Gero
612
2BBdet
22
22
=
−+−
−−ω ω
ω ω
mk mk
mk mk % w"i&" ield$
( ( ( ( 6122BB 2222 =−−+−− ω ω ω ω mk mk mk mk (C)
Equation (C) &an be $impli!ied to
61F12 2242 =+− k mk m ω ω % (16)
3"ere!ore t"e natural !requen&ie$ remain t"e $ame a$ be!ore' =owe#er% t"e natural mode$o! t"e $$tem-
( )
( )
(( )
4'62BB
2B2B
B
2B
2
1
2
1
1
2
1
1 =−−
−−=
−
−=
ω
ω
mk
mk
X
X and
( )
( )
(( )
4'22BB
2B2B
B
2B
2
2
2
2
2
2
2
1 −=+−
+−=
−
−=
ω
ω
mk
mk
X
X '
(11)
1$t mode $"ape 2nd mode $"ape
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+art III- Natural !requen&ie$ remain t"e $ame% but equation$ o! motion and mode $"ape$are di!!erent' 3"e !ir$t &a$e i$ $tati& &oupling and t"e $e&ond i$ bot" dnami& and $tati&&oupling'