Synchronous machines: Protection relevant basics
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Synchronous machines:
Protection relevant basics
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Synchronous Machine without Load
~
Xd IG
Vp V
Vp = V + j·IG·XdTurbine
ExcitationSystem
AVRn
n+n-
Speed-Control
V+V-
50 HzS →∞
V
IG
VP V
1/xd
IExc 0
IG= 0
Im
Re
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Synchronous Machine connected to the Net:inductive Load
~
Xd
IG
Vp V
Vp = V + j·IG·Xd
TurbineExcitationSystem
AVRn
n+n-
Speed-Control
V+V-
50 HzS →∞
V
IG
Re
φ = +90°δ=0°
1/xd
IExc
IG
VP j·IG·Xd
V
Im
(Different scales for IExc and IG)
V= VN, f = fN
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Synchronous Machine connected to the Net:capacitive Load
~
Xd
IG
Vp V
Vp = V + j·IG·Xd
φ = -90°δ=0°
1/xd
IExc
IG
VP
j·IG·Xd V
Re
Im
TurbineExcitationSystem
AVRn
n+n-
Speed-Control
V+V-
50 HzS →∞
V
IG
(Different scales for IExc and IG)
V= VN, f = fN
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Synchronous Machine connected to the Net:active Load
~
Xd IG
Vp V
Vp = V + j·IG·Xd
φ = 0°
δ
1/xd
IExc IG
Re
VP
j·IG·Xd
V
Im
TurbineExcitationSystem
AVRn
n+n-
Speed-Control
V+V-
50 HzS →∞
V
IG
(Different scales for IExc and IG)
V= VN, f = fN
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Synchronous Machine connected to the Net:rated Load
~
Xd
IG
Vp V
Vp = V + j·IG·Xd
TurbineExcitationSystem
AVRn
n+n-
Speed-Control
V+V-
50 HzS →∞
V
IG
φNδ
1/xd
IExc N
ING
VP
j·IG·Xd
V
Im
Re
(Different scales for IExc and ING)
V= VN, f = fN
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Synchronous Machine in Island operationat VN and fN , partial loaded
~
Xd
IG
Vp V
Vp = V + j·IG·Xd
TurbineExcitationSystem
AVRn
n+n-
Speed-Control
V+V-
50 HzS →∞
V
IG
φδ
1/xd
IExc
IG
VP
j·IG·Xd
V=VN
Im
Re
(Different scales for IExc and IG)
V= VN, f = fN
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Synchronous Machine in Island operation
~
Xd
IG
Vp V
Vp = V + j·IG·Xd
TurbineExcitationSystem
AVRn
n+n-
Speed-Control
V+V-
50 HzS →∞
V
IG
φδ
1/xd
IExc
IG
VP
j·IG·Xd
V
Im
Re
(Different scales for IExc and IG)
V= >VN, f = fN
VN
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Synchronous Machine in Island operation
~
Xd
IG
Vp V
Vp = V + j·IG·Xd
TurbineExcitationSystem
AVRn
n+n-
Speed-Control
V+V-
50 HzS →∞
V
IG
φδ
1/xd
IExc
IG
VP
j·IG·Xd
V=VN
Im
Re
(Different scales for IExc and IG)
V= VN, f = >fN
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Synchronous Machines: P-Q-Equations describing the Theoretical Stability Limit
sinx
UE
Pd
ϑ
⋅
=
Salient-pole machine
ϑ ϑ sin2xx
x-x
2
U sin
x
UE P
qd
qd2
d
+⋅
=
)sinx
x-x (1
x
U cos
x
UE Q 2
q
qd
d
2
d
ϑ ϑ +−⋅
=
P active power [p.u.]Q reactive power [p.u.]E (VP) pole wheel voltage (e.m.f.) [p.u.]U (V) terminal voltage of the generator [p.u.]xd synchronous direct axis reactance [p.u.]x
qsynchronous quadrature axis reactance [p.u.]
ϑ pole wheel angle
Cylindrical-rotor machine (xd ≈≈≈≈ xq)
x
U cosx
UE Q
d
2
d−
⋅= ϑ
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Construction of the Stability Limitsfor a Salient-Pole Machine
3.5 3 2.5 2 1.5 1 0.5 0 0.5 1
0.5
0.5
1
1.5
22.0
0.5
P 1i
P 3i
P 5i
P 6i
P dy1i
P dy2i
Sthya
Sprya
Stdya
cosφ
13.5 Q 1iQ 3i, Q 5i
, Q 6i, Q dy1i
, Q dy2i, Sthx
a, Sprx
a, Stdyx
a, Q N,
Theoretical staticstability limit
Dynamicstability limit
Practical staticstability limit
P[p.u]
1/xd
1/xq
Q[p.u]
1/x’d
E=0
E’=0
E=1,68
E’=0,25
E=1,0
E=0,5
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Capability Curve of a Salient-Pole Generator (1/2)
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Capability Curve of a Salient-Pole Generator (2/2)
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Construction of the Stability Limitsfor a Cylindrical-Rotor Machine
3 2.5 2 1.5 1 0.5 0 0.5 1
0.5
0.5
1
1.5
22.0
0.5
P 1i
P 3i
P 6i
P dy1i
P dy2i
Sthya
Sprya
Stdya
cosφ
Theoretical staticstability limit
Dynamicstability limit Practical static
stability limit
P[p.u]
1/xd Q[p.u]
1/x’d
E=0,8
E’=0
E’=0,4
E=2,51
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Capability Curve of a Turbo Generator
type of generator: TLRI 108/46
nominal apparent powerS N = 200 MVA
nominal voltage V N = 15.750 kVnominal current I N = 7.331 kAnominal frequency f N = 50.0 Hzpower factor cos ϕN = 0.8cold-air temperature T x = 40.00 °C
MVAr 140 120 MVAr100 80 60 40 20 0 20 40 60 80 100 120 140 160 180
underexcited overexcited
Q
P
MW
220
200
180
160
140
120
100
80
60
400,2
0,4
0,6
0,7
0 , 8
0 , 8
5
0 , 9
0 , 9
5
0 , 9
7 5
0 , 9
7 5
0 , 9
5
0 , 9
0,2
0,4
0,6
0,7
0,8
0,85
C o s φ
C o s φ