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2014
© Trade Science Inc.
ISSN : 0974 - 7435 Volume 10 Issue 24
BioTechnology
An Indian JournalFULL PAPER
BTAIJ, 10(24), 2014 [15049-15059]
Novel MC-DTC control method for induction motor based on space vector modulation
Cai Bin-jun1,2, Nian Xiao-hong1,*
1School of Information Science and Engineering, Central South University, Changsha 410004, (P.R.CHINA)
2College of Electrical & Information Engineering, Hunan Institute of Engineering, Xiangtan 411101, (P.R.CHINA)
E-mail : [email protected]
ABSTRACT This paper presents a novel MC-DTC method for fed induction motor based on spacevector modulation. The advantages of DTC method are combined with the advantages ofthe matrix converter based on space vector modulation technique. This proposed novelmethod provides a precious input power factor control capability beside the high controlperformances. Furthermore, Conventional principles of DTC and MC were described. Thecombination of the DTC and MC were given in details. The simulation and experimentresearch were carried out to identify the new method effectiveness. The results ofinduction motor control at steady state are shown to improve the low-speed performanceand strong adaptability of this novel control strategy. KEYWORDS Matrix converter; DTC; Induction motor; Space vector modulation; Low-speedperformance.
15050 Novel MC-DTC control method for induction motor based on space vector modulation BTAIJ, 10(24) 2014
INTRODUCTION
In two recent decades, due to the need to increase the quality and the efficiency of the power supply and usage, three phase matrix converter becomes a modern energy converter. The research of matrix converter has been carried on with many theoretical[1],[2],[3].These achievements along with the emergence of bidirectional switch make it possible to apply the matrix converter to practical applications. Various methods to control the matrix converter have been proposed [4],[5], being the scalar modulation and the indirect space vector modulation widely used. It fulfills all requirements of the conventionally used rectifier/dc link/ inverter structures. Some advantages of the matrix converter can be seen as following: the use of a compact voltage source, providing sinusoidal voltage with varying amplitude and frequency besides the sinusoidal input current and unity input power factor at power supply side. Matrix converter has a simple topology and a compact design due to the lack of dc-link capacitor for energy storage.
Since the DTC method has been proposed in the middle of 1980’s, DTC method becomes one of the high performance control strategies for AC machine to provide a very fast torque and flux control[6][7]. There are no requirements for coordinate transformation, no requirements for PWM generation and current regulators. It is widely known to produce a quick and fast response in AC drives by selecting the proper voltage space vector according to the switching status of inverter which is determined by the error signal of reference flux linkage and torque with their estimated values and the position of the estimated stator flux. Some research is being done to adapt DTC to new converters and also to reduce the torque ripple, which is one of its main drawbacks. DTC is the direct control of torque and flux of a drive by the selection, through a look-up table, of the inverter voltage space vectors. The main advantage of DTC is its structure, no coordinate transformations and no PWM generation are needed. However, torque and flux modulus values and the sector of the flux are needed. Not only it is a very simple and robust signal processing scheme but also a very quick and precise torque control response is achieved.
In this paper, a novel MC-DTC method for fed induction motor based on space vector modulation is proposed. The advantages of DTC method are combined with the advantages of the matrix converter based on space vector modulation technique.The appropriate switching configurations of the matrix converter for each constant time are presented in an opportune switching table[8],[9],[10]. The table is only entered by the imaginary voltage vector, which is generated from the DTC method for voltage source inverter, and the position of input voltage vector which can be measured exactly. Simulation and experiment at the high-speed and low-speed are carried out to prove the good performances of the novel method.
CONVENTIONAL DIRECT TORQUE CONTROL
Mathematical mode of induction machine
The mathematical mode of induction machine is shown in Figure 1.
Figure 1 : The mathematiacal mode of induction motor
According to Figure 1 flux-linkage equations of induction machines in the stator stationary reference frame as follows.
( )s s s sv R i dtα α αψ = −∫ (1)
( )s s s sv R i dtβ β βψ = −∫ (2)
Where sαψ and are theα -axis and β -axis component of sψ
r respectively; svα and svβ are the α -axis and β -axis
component of svr
respectively; siα and siβ are theα -axis and β -axis component of sir
. The electromagnetic torque can be expressed using the following equation.
3 3( ) ( )2 2e p s s p s s s sT n i n i iα β β αψ ψ ψ= × = −
rr (3)
Where eT is electromagnetic torque and pn is the number of rotor pole pairs.
sβψ
BTAIJ, 10(24) 2014 Cai Bin-jun and Nian Xiao-hong 15051
Principle of DTC The basic principle in conventional DTC for induction motors is to directly select stator voltage vectors by means of
a hysteresis stator flux and torque control. As it is shown in Figure 2.
*sψ
sψψE
ψH
TeH
*eT
eT
TeE
SASBSC
eT
sψ AIBI
rω
Figure 2 : The diagram block of basic DTC
From Figure 2 can obtain stator flux *sψ and torque *
eT references are compared with the corresponding estimated values. Both stator flux and torque errors, ψE and TeE , are processed by means of a hysteresis band comparators. In particular, stator flux is controlled by a two-level hysteresis comparator, whereas the torque is controlled by a three-level comparator. On the basis of the hysteresis comparators and stator flux sector a proper VSI voltage vector is selected by means of the switching table given in Table 1.
TABLE 1 : Basic DTC switching table
MC SPACE VECTOR MODULATION
Working principle of MC MC is an AC-AC converter, with mxn bidirectional switches, which connects an m-phase voltage source to an n-phase load. The three-phase, 3x3 switches, MC shown in Figure 3 is the most interesting. It connects a three phase voltage source to a three-phase load[11].
Figure 3 : The topology of matrix converter
In the MC shown in “Fig.3,” siv , { }, ,i A B C= are the source voltages, sii , { }, ,i A B C= are the source currents. jNv ,
{ }, ,j A B C= are the load voltages, ji , { }, ,j A B C= are the load currents, iv , { }, ,i A B C= are the MC input voltages and ii ,
{ }, ,i A B C= are the input currents. A switch, ijS , { }, ,i A B C= , { }, ,j a b c= can connect phase i of the input to phase j of
the load. With a suitable switching strategy, arbitrary voltages jNv at arbitrary frequency can be synthesized. Switches are characterized by the following equation.
01
ijij
ij ij
witch S is openS
witch S S close⎧⎪= ⎨⎪⎩
(4)
A mathematical model of MC can be derived from “Fig.3” as follows:
1
D
b
D
sio
z
d d d Wm
15052
The coDC and DC-AC
The cobidirectional sw
DC-AC conver 6 pow
space vector Us 60 degrees. T
output , ,A B C a The ou
Any ezero output vol
Where
MM TTd δ ==
NN mTTd δ ==
M ddd −−=10
Where ,M NT T modulation ind
No
onventional thrC. It is shown i
ontrol signal fowitches corresp
rter space vecwer switches of
1 6U U− and 2 zThey constituteand the input Dutput voltage a
expected outpultage 0U or 7U
e NM dd , and
( Jvm θ−060sin
Jvm θsin
N
is the switchindex of output vo
ovel MC-DTC con
⎢⎢
⎣
⎡
vvv
cN
bN
aN
(((⎢
⎢
⎣
⎡
iii
C
B
A
ree-phase to thin Figure 4.
Figure
for bidirectionapond to a 3x3 m
ctor modulatiof inverter with ero vector 0 ,Ue 6 uniform seDC , such as M
and the corresp
Figure 5 :
ut voltage spac. Suppose the
U
0d are the ratio
)J (8)
(9)
(10)
ng time of vecoltage. And
ntrol method for in
( )( )( )
( )( )( )⎢
⎢
⎣
⎡=
⎥⎥
⎦
⎤
tStStS
ttt
Ac
Ab
Aa
N
N
N
( )( )( )
( )( )( )⎢
⎢
⎣
⎡=
⎥⎥
⎦
⎤
tStStS
ttt
Ca
Ba
Aa
hree-phase matr
e 4 : The topol
al switches commatrix in each s
on 8 possible com
7,U . The phasegments. The th
101M = whichponding switchi
The output vo
e vector JU isangle between
dUdU MMJ +=
o cycles of MU
ctors MU and
nduction motor ba
( ) (( ) (( ) ( )tStS
tStStStS
CcBc
CbBb
CaBa
( ) ( )( ) ( )( ) ( )⎥
⎥tStStStStStS
CcCb
BcBb
AcAb
rix converter’s
logy of 3x3 m
me from the coswitching perio
mbinations showe angle betweehree digits in bh represents theing states are r
oltage vector a
formed by ad
n JU and MU
00UdUd NN +
NM U, and 0U r
MU respectiv
ased on space vect
)))
( )( )( )⎥⎥
⎦
⎤
⎢⎢
⎣
⎡⋅⎥⎥
⎦
⎤
tvtvtv
C
B
A (5)
) ( )( )( )⎥⎥
⎦
⎤
⎢⎢
⎣
⎡⋅⎥⎥
⎦
⎤
tititi
c
b
a (6)
modulation pr
matrix convert
ontrol circuit aod.
wn in Figure 3en one effectivebrackets exprese switching of trepresented in F
and switching
djacent two basis Jθ .
(7)
respectively. A
vely. Tδ is the
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rocess consists
ter
and drive circu
3 are correspone voltage spacess the linking sthe switches SFigure 5.
g states
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And
switching per
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BTAIJ, 10(24) 201
Where omU an1=cm ,φ is the
When adjacent basic v
AC-DC conver The sp
opology is reprectification, th
MC space vect Three-
possible switchTable 2: group nput phase, gr
each SCs, the crepresented in F
Novel DTC-M The no
DTC for matridesired imagina
14
nd imU are the e input power fthe rotating sp
voltage space v
rter space vecpace vector mpresented in th
he DC voltage
tor modulatio-phase matrix hing configura
I (±1, ±2, …,roup II (0a, 0b, corresponding Figure 6.
MC based on SVovel DTC-MCix converter[12ary non-zero V
vm
amplitude of ofactor angle. pace vector JUvectors constitu
ctor modulatiomodulation proc
he left dotted is.
dU
n converter mo
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Figure 6 : (a
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VSI voltage vec
Cai Bin-ju
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output and inpu
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odule includes nly 21 SCs caof the SCs whif the SCs whic-neutral voltag
a) The output v
TABLE 2 : MC
apply the directding to the inctor, the two no
un and Nian Xiao-
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ut voltage, cm
segment, the lment and one ze
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osϕ
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t SVM techniqnput voltage linon-zero voltage
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(11)
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ocal average oero voltage spa
ly similar to the correspondin
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he intput line
ero vectors
que to overcomne to neutral ve vectors will b
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he modulation ng formulas ar
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rent vector hav
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me the disadvanvector sector lbe selected.
ation index, ge
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Figure 6. Thhm for MC ashe same one o
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15053
enerally set
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ere are 27 s shown in of the other phase. For rections as
onventional ombine the
15054 Novel MC-DTC control method for induction motor based on space vector modulation BTAIJ, 10(24) 2014
The criteria utilized to implement the switching patterns for the matrix converter can be explained referring to the following example.
We can assume the imaginary VSI voltage vector is 1V , and the input voltage lint-to-neutral vector [14],[15] is located in sector 1 as shown in Figure 7.
Figure 7 : Block diagram of novel DTC-MC based on SVM
From Table 2, in order to generate a voltage vector in the same direction of 1V , there are 6 possible SCs (±1, ±2, ±3). According to the input voltage vector location, there are only 3 SCs having the voltage vectors as same direction to 1V : +1, -2 and -3. To synthesize the input current vector to be in phase with the input voltage vector located in sector 1, two SCs finally selected are +1 and -3. The switching table based on these criteria is shown in Table 3.
TABLE 3 : MC-DTC switching table using SVM
As shown in Figure 7, the output voltage of matrix converter for each SCs is calculated.
aA aB aC a a
S bA bB bC b b
cA cB cC c c
S S S V VV S S S V T V
S S S V V
⎡ ⎤ ⎡ ⎤ ⎡ ⎤⎢ ⎥ ⎢ ⎥ ⎢ ⎥= =⎢ ⎥ ⎢ ⎥ ⎢ ⎥⎢ ⎥ ⎢ ⎥ ⎢ ⎥⎣ ⎦ ⎣ ⎦ ⎣ ⎦
(13)
Where the switching function ijS is 1 when the switch joining input line i to output line J is ON and i is 0 otherwise,
, ,i a b c= and = , ,J A B C . Matrix T represents the status of each switching configuration in Table 2. The input voltage vector of induction motor in the stationary reference frame for each sampling period.
1 2
1 112 2 23 3 30
2 2
asd
s x y bsq
C
Vv
v t T t T Vv
V
⎡ ⎤ ⎡ ⎤− −⎢ ⎥⎡ ⎤ ⎢ ⎥⎢ ⎥ ⎡ ⎤= = +⎢ ⎥ ⎣ ⎦ ⎢ ⎥⎢ ⎥⎣ ⎦ ⎢ ⎥⎣ ⎦⎢ ⎥⎣ ⎦
(14)
From Figure 6, the duty ratios of the two non-zero Scs. are calculated as follows.
1 2
21
1 2
sin( 6 ) sin( 6 )1
x y VSI
yx
i i
t V t V Vt Vt V
t tπ α π α
+ =
=− +
+ =
(15)
B
T
pc
thc
T
r
w
BTAIJ, 10(24) 201
(
(
1
2
sinco
sinco
t
t
π
π
=
=
The in
The m
The simulation In ord
period of 50μs.cage induction
=2.2nP kw ,U
The w
he matrix outpcurrent is calcu
The simulation At the
reference 0.6w Figure
waveform.
14
)( )
)( )
6os
6os
i
i
i
i
π αα
π αα
−
+
nduction motor
motor estimated
n model of MCder to verify th
The system simotor:
=380nU v , =4sR
whole system haput voltages anulated on the ba
n result of MCe high speed o
wb . The simulate 9 shows a go
(16
r stator flux can
d torque can be
SIMU
C-DTC based e behavior of timulation mod
.35Ω , =0.43rR Ω
as been simulad the input curasis of the matr
Figure 8 : T
C-DTC based operation, indution result show
ood performanc
Figu
Cai Bin-ju
6)
n be obtained f
(s s s sv R iϕ = −∫)
e obtained.
(32
psd sq
nT iϕ= −) )
ULATION OF
on SVM the proposed s
del is shown in
Ω , =2sL mH , rL
ated using the Srrents respectivrix input curren
The simulatio
on SVM uction motor iw in Figure 9-Fce in terms of
ure 9 : Flux at
un and Nian Xiao-
from the calcul
)s dt
)sq sdiϕ− )
MC-DTC BA
scheme, some Figure 8. The
=2r mH , =69mL
Simulink packvely, thus assunt.
n model MC-D
is running at Figure 10. stator flux. As
100rpm , 25Nm
-hong
lated input volt
(17)
(18)
ASED ON SVM
simulation hasmachine utiliz
9.31mH , 0.0J =
kage. Equation uming ideal sw
DTC based on
speed 1000rpm
s it can be seen
for MC-DTC
tage and the m
M
s been carried zed for simulati
2089kg m⋅ , =2P
(5) and Equatiwitching device
n SVM
m , rated load
n in Figure 9, s
C
easured stator
out assuming aions is a three-
.
ion (6) are usees. The mains f
torque 25Nm
stator flux show
15055
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a sampling -phase 3kw
d to obtain filtered line
m and flux
ws a circle
1
Fs
r
cc
7fc
15056
FigureFurthermore, thsystem with reg
At thereference 0.6 w
Figurechange as a stecurrent wavefo
The n7.5kw MC. Thefour-step commcontrolled hyste
No
e 10 shows stathe stator curregard to the impe low speed op
wb . The simula
e 12 shows theep command frrms are almost
novel method he MC-DTC algmutation proceeresis brake pr
ovel MC-DTC con
Figure 10 : C
tor flux and elents have sinuplementation ofperation, induc
ation result show
Figur
Figure 13 :
e dynamic perfrom 25Nm+ tot sinusoidal im
EXPE
had been testegorithms were ess, required wrovides the load
ntrol method for in
Current flux a
ectromagnetic usoidal wavefof the novel MCction motor isw in Figure 11
re 11 : Flux at
Torque, curre
formances of tho 25Nm− . The
mmediately righ
ERIMENT OF
d. The parameimplemented
when bidirectiod torque. A blo
nduction motor ba
and torque at
torque of the
orms. This figC-DTC methods running at a- Figure 12.
t 100rpm , 25Nm
ent and flux at
he novel contre electromagneht after the step
F MC-DTC BA
eters are samein a TMS320Lonal switches ock diagram of
ased on space vect
1000rpm for M
induction motogure emphasized.
very low spee
for MC-DTC
t 100rpm for M
rol method at thetic torque shop command.
ASED ON SVM
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f the system set
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or fully followes the good p
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C
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he rotor speedows a very goo
M
n parameters. Tachieving a sams implementedtup is shown in
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The motor wample period of d in a FPGA. n Figure 13.
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BTAIJ, 10(24) 201
At thereference 0.6w
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Figure 15 : DuDTC
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14
e high speed owb . The experim
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Figure 13 :
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Figure 14 :
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uction motor iow in Figure 14
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ure 15, electrome proposed novhe type of the re identical to tas security lim
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15057
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15058
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ProjecResearch Fund
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2] Ding wei2002,24(2
3] Lan zhiyojournal of
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ovel MC-DTC con
Figure
torque step co
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a new DTC-SVthe SVM methrequirements i
e shown to valiut current harmlux and torque
61075065, 613vincial educati
in,“New mo,2006,23(4):54“Matrix conv
in, “Simulationversity, 2010,27
ntrol method for in
(Wb)
sΒ
ψ
16 : The flux
ommand from
stator flux,torqce a re-design
of the torque riThe standard d
CO
VM method fohod on matrixis suggested. Tidate the effec
monic spectrumsmall and stab
ACKNO
321003, 51177on department
RE
dulaiton strate2-546. erter and its r
n reearch of th7(3):110-115.
nduction motor ba
(Wb)sαψ
at 100rpm , 25N
m 25Nm+ to 2−
que in the low of the MC inp
ipple with respdeviation of the
ONCLUSION
or matrix conv
x converter. A The simulation tiveness of the
m and low-speeble. It has adva
OWLEDGMEN
7040 supportedt.
FERENCES
egy on raising
research situati
hree phase to t
ased on space vect
Nm for MC-DT
5Nm the torqu
frequency rangut filter would
pect to both thee torque was ca
verter. The advnew switchingand experimen
e new control sed performanceantages and goo
NTS
d by NSFC/Pr
g voltage trans
ion,” natural s
three phase spa
tor modulation
TC
ue,current and
ge when compd be enough to oe torque referenalculated to me
vantages of theg table for thent results on thscheme. Furthee as compared od future, it is w
roject 13B014
sfer ratio for m
science journa
arse matrix con
BTAIJ,
d flux at 100rpm
ared with the hovercome this nce and the moeasure the torqu
e DTC method e DTC-SVM whe induction mermore, the novto the conventworth further s
Supported by
matrix convert
al of xiangtan
nverter,” natur
J, 10(24) 2014
m for MC-
high speed. drawback. otor speed, ue ripple.
have been which fully motor at the
vel control tional DTC studying.
y Scientific
ter,”control
university,
ral science
BTAIJ, 10(24) 2014 Cai Bin-jun and Nian Xiao-hong 15059
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