useful trigometric identities
TRANSCRIPT
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
Session 13; Page 1/15
Spring 2004
Useful Trigometric Identities in AC Machine Analysis
1. sin
2
+ cos
2
= 12. sin = sin cos cos sin
3. cos = cos cos sin sin
4. Acos + Bsin = A2 B2 sin , = tan 1 A B
5. Acos + Bsin = A2 B2 cos , = tan 1 B A
6. sin cos = 12
[sin + sin
7. cos cos =12 [cos + cos
8. sin sin = 12
[cos - cos
9. cos + cos 23
+ cos 23
= 0
10. sin + sin 23
+ sin 23
= 0
11. sin cos + sin 23
cos 23
+ sin 23
cos 23
0
12. cos2
+ cos2
23 + cos
2
23
3
2
13. sin2 + sin2 23
+ sin2 23
= 32
14. cos cos 23
+ cos 23
cos 23
+ cos 23
cos 34
15. sin sin 23
+ sin 23
sin 23
+ sin 23
sin 34
16. sin cos 23
+ sin 23
cos + sin 23
cos 23
3 34
17. sin cos 23
+ sin 23
cos 23
+ sin 23
cos = 3 34
18. cos cos + cos 23
cos 23
+ cos 23
cos 23
= 32
cos
19. sin sin + sin 23
sin 23
+ sin 23
sin 23
= 32
cos
20. sin cos + sin 23
cos 23
+ sin 23
cos 23
= 32
sin
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
Session 13; Page 2/15
Spring 2004
Synchronous Machine Windings
G
C
C
B
B
A
Quadrature Axis
Direct
Axis
Reference
D
F
Q
Q
F
D
A
Transient Model for a Synchronous Machine
Generator Convention
G
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
Session 13; Page 3/15
Spring 2004
Notation
f can represent i, v, .
f
= r rotating reference frame fixed on the rotor
s stationary reference frame fixed on the stator
= s stator quantity
r rotor quantity
a A-Phase quantityb B-Phase quantity
c C-phase quantity
d direct-axis quantity
q quadrature-axis quantity
F field quantity
D direct-axis damper winding quantity
Q quadrature-axis damped winding quantity
g eddy current winding quantity
l leakage quantitym mutual quantity
= rotor quantities referred to the stator
(superscript on the subscript)
fabc
fa
fbfc
; fr
dq0
frd
fr
qfr0
F denotes that the quantity F is a complex vectorF denotes that the quantity F is a phasor
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
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Spring 2004
Inductances
Stator Flux Linkage Equations:
abc Lsiabc LsriFDgQ
Rotor Flux Linkage Equations:
FDgQ LTsriabc LriFDgQ
Combined Stator and Rotor Flux Linkage Equations:
abcFDgQ
Ls LsrLTsr Lr
iabciFDgQ
a
b
c
F
D
g
Q
Laa Lab Lac LaF LaD Lag LaQ
Lba Lbb Lbc LbF LbD Lbg LbQ
Lca Lcb Lcc LcF LcD Lcg LcQ
LFa LFb LFc LFF LF D LF g LFQ
LDa LDb LDc LDF LDD LDg LDQ
Lga Lgb Lgc LgF LgD Lgg LgQ
LQa LQb LQc LQF LQD LQg LQQ
ia
ib
ic
iF
iD
ig
iQ
where
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
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Spring 2004
Stator Self-inductances
Laa
Ls
Lm
cos2d
Lbb Ls Lmcos2 d 2 3
Lcc Ls Lmcos2 d 2 3
Stator Mutual-inductances
Lab Lba Ms Lmcos2 d 6
Lbc Lcb Ms Lmcos2 d 2
Lca Lac Ms Lmcos2 d 5 6
Rotor Self-inductances
LF
LD
Lg
LQ
Rotor Mutual-inductances
LFD
LDF
Mrd
LgQ LQg Mrq
LFg LgF LDg LDg 0
LFQ LQF LDQ LDQ 0
Stator-rotor Mutual-inductances
LaF LFa MFcosd
LbF LFb MFcos d 2 3
LcF LFc MFcos d 2 3
LaD LDa MDcosd
LbD LDb MDcos d 2 3
LcD LDc MDcos d 2 3
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
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Spring 2004
Lag
Lga
Mgcos
d
Lbg Lgb Mgcos d 2 3
Lcg Lgc Mgcos d 2 3
LaQ LQa MQsind
LbQ LQb MQsin d 2 3
LcQ LQc MQsin d 2 3
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
Session 13; Page 7/15
Spring 2004
Parks Transformation
frodq R r P 0 fabc
where r r2
Coordinate axis transformation
P 0 :2
3
1
2
1
2
1
2
1 1
2
1
2
0 323
2
abc odq
Transformation to rotating reference frame
R r :
1 0 0
0 cosr sin r0 sinr cos r
0dqs 0dqr Rotation
Combine into one step
P r R r P 0
fr0dq P r fabc
fr0
frd
frq
2
3
1
2
1
2
1
2
cosr cos r23 cos r
23
sinr sin r23 sin r
23
fa
fb
fc
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Power Systems Analysis
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Spring 2004
P r :2
3
1
2
1
2
1
2
cosr cos r23 cos r
23
sinr sin r23 sin r
23
P 1 r PT r
P 1 r2
3
1
2cosr sinr
1
2cos r
23 sin r
23
1
2cos r
23 sin r
23
P rdP 1 r
dt
0 0 0
0 0
0 0
: x
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
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Spring 2004
Synchronous Machine Equations
1. Stator Voltage Equations: (Note: p = d/dt)
vabcs rsiabcs pabcs
v0dqs rsi0dqs p0dqs x0dqs
2. Rotor Voltage Equation:
vFDgQr RriFDgQr pFDgQr
3. Stator Flux Linkage Equations:
abcs Lsiabcs LsriFDgQr
odqs Lsiodqs LsriFDgQr
4. Rotor Flux Linkage Equations:
FDgQr LTsriabcs LriFDgQr
FDgQr LT
sriabcs LriFDgQr
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
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Spring 2004
0s
ds
qs
Fr
Dr
gr
Qr
L0
0 0 0 0 0 0
0 Ld 0 kMF kMD 0 0
0 0 Lq 0 0 kMg kMQ
0 kMF 0 LF MD 0 0
0 kMD 0 MD LD 0 0
0 0 kMg 0 0 Lg MQ
0 0 kMQ 0 0 MQ LQ
i0s
ids
iqs
iFr
iDr
igr
iQr
k3
2
TE idq iqd
p3 t i0 v0 id vd iq vq
Ea0MFiFe
j
2
Ea
Ea0MFiF
2
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
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Spring 2004
Synchronous Machine Parameters
Xd
direct axis reactance
Xq quadrature axis reactance
Xd direct axis transient reactance
Xq quadrature axis transient reactance
Xd direct axis subtransient reactance
Xq quadrature axis subtransient reactance
X2 negative sequence reactance
X0 zero sequence reactance
rsdc stator dc resistance
rsac stator ac resistance
rf r field resistance referred to the statorr2 negative sequence resistance
Td0 direct axis open-circuit transient time-constant
Td direct axis short-circuit transient time-constant
Td direct axis short-circuit subtransient time-constant
Ta armature short-circuit (d.c.) time-constant
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
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Spring 2004
Machine Turbo Hydro Synchronous Synchronous
Constant Generator Generator Condensor Motor
Xd 1.1 1.15 1.80 1.20
Xq 1.08 0.75 1.15 0.90
Xd 0.23 0.37 0.40 0.35
Xq 0.23 0.75 1.15 0.90
Xd 0.12 0.24 0.25 0.30
Xq 0.15 0.34 0.30 0.40
X2 0.13 0.29 0.27 0.35X0 0.05 0.11 0.09 0.16
rsdc 0.003 0.012 0.008 0.01
rsac 0.005 0.012 0.008 0.01
r2 0.035 0.100 0.05 0.06
Td0 5.6 5.6 9.0 6.0
Td 1.1 1.8 2.0 1.4
Td 0.035 0.035 0.035 0.035Ta 0.16 0.15 0.17 0.15
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UI: EE422/NTU: PS 512-S
Power Systems Analysis
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Spring 2004
Hydro Generator (salient pole rotor)
Xmd 0kMD Xmq 0kMQ
Xd 0Ld Xmd Xld s
Xq 0Lq Xmq Xlqs
XdXmdXl f r
Xmd
Xl f r
Xld s
Xq Xmd Xld s
XdXmdXld r Xl f r
XmdXl f r Xl f r Xld r Xld r XmdXld s
XqXmqXlqr
Xmq XlqrXlqs
X2Xd Xq
2
X0Xld Xlq
2
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Power Systems Analysis
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Spring 2004
Td01
rf r
Xmd Xl f r
b
TdXdXd
Tdo
TdXdXd
Tdo
Tq
Xq
Xq Tqo
Ta1
rsb
2XdXq
Xd Xq
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Power Systems Analysis
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Spring 2004
Three Phase Short Circuit of a Synchronous Machine
ias t 2 Ea1
Xd
1Xd
1Xd
et
Td
1X
d
1X
de
t
Td sin et
2 Ea12
1Xd
1Xq
et
Ta sin
2 Ea12
1Xd
1Xq
et
Ta sin 2et
Name Magnitude Frequency T
Steady Ea1
XdFundamental
Transient Ea1
Xd
1Xd
Fundamental Td
Subtransient Ea1
Xd
1Xd
Fundamental Td
Asymmetrical Ea12
1X
d
1Xq
sin Zero Ta
Second Harmonic Ea12
1Xd
1Xq
Double Fundamental Ta