TRANSMISSION &
DISTRIBUTION
A Division of Global Power
POWER SYSTEM STABILITY CALCULATION TRAINING
D1
BiPiil
Day
1
- Bas
i
c Pr
i
ncip
l
es
•
July4,2013
Prepared by: Peter Anderson
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OUTLINE
2
OUTLINE
• Definitions of Stability
T f St bilit
•
T
ypes o
f
St
a
following a given disturbance or a set of disturbances
following
a
given
disturbance
,
or
a
set
of
disturbances
,
the system state stays within specified bounds and the
system reaches a new stable equilibrium state within a
ifid id fti
spec
ifi
e
d
per
i
o
d
g
e
q
uilibrium after bein
g
sub
j
ected to a
pgq gj
p
hysical disturbance, with most system variables bounded so
that practically the entire system remains intact
It is not necessary that the system regains the same steady state
ti ilib i i t th di t b Thi ld b th
opera
ti
ng equ
ilib
r
i
um as pr
i
or
t
o
th
e
di
s
t
a
change
in system topology or structure.
It is important that the final steady state operating equilibrium after the
fault is steady state acceptable. Otherwise protections or control
actions could introduce new disturbances that might influence the
actions
could
introduce
new
disturbances
that
might
influence
the
stability of the system. Acceptable operating conditions must be
clearly defined for the power system under study.
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Pow er Flow
FaultCurrents
Long ‐TermStability
Short‐TermStability
Stato rTransi ents
Resonance/Saturation
Resonance/Saturation
Switching
Lightning
Time (s)
Time
(s)
1.E‐06 1.E‐03 1.E+00 1 .E+03
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ANGULAR STABILITY
7
ANGULAR
STABILITY
The ability of the Synchronous Machines
within a Power System to remain In
Synchronism following a disturbance
Large Disturbances (Transient Stability)
Small Disturbances (Small
signal or Dynamic
Small
t
ore
th
e
S
ys
t
em
Frequency to within an acceptable range
following a disturbance
following
a
disturbance
Short
-
Term (Governor action)
Short
-
Term
(Governor
action)
Long-Term (Turbines, Boilers, Nuclear Reactors)
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VOLTAGE STABILITY
it
s
Local in nature since it is difficult to transport
Local
in
nature
since
it
is
difficult
to
transport
reactive power through the network (X>>R)
Short-Term (1-5 s Induction motors, Electronically
controlled loads, HVDC converters)
controlled
loads,
ow
Transit from State
-
A to State
-
A
’
: Stability Analysis
Transit
from
State
-
A
to
State
-
A:
Stability
Analysis
Transit from State-A’ to State-B: Stability Analysis
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SYNCHRONOUS MACHINES
11
SYNCHRONOUS
=P
d
1.2
1.4
04
0.6
0.8
1
Powe r(pu)
0
0.2
0
.
4
0 30 60 90 120 150 180
LoadAngle(deg)
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STEADY
STATE OPERATIONAL LIMITS
13
STEADY
-
STATE
OPERATIONAL
LIMITS
Limiting Factors:
Stator Current Thermal Limit
•
it
•Dependent on Exciter Speed of Response
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OPERATIONAL LIMITS FOR SYNCHRONOUS
14
GENERATORS
Xd=2.0pu
SCR=0.5
Powerfactor=0.8
Exciter No‐loadMargin Full‐loadMargin
Slow‐Actin
g
35% 20%
g
Fast‐Acting 20% 10%
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OPERATIONAL LIMITS FOR SYNCHRONOUS
15
GENERATORS
Stator Current Limit
1.25
Stator
Current
Limit
I
rated
=1.0pu
Centre = 00
Q
Field
Current
Limit
I
Frated
=√{(SCR+sinθ)
2
+cosθ
2
}
Centre = 0
‐
SCR
05
0.75
1
Q
Centre
=
0
,
‐
SCR
Radius=I
Frated
Q
Rotor
Angle
Stability
Limit
LowerFieldVoltage=LessStability
Fast‐actingExciter:
0.25
0.5
0.75
NLMargin(NLM)=0.2
FLMargin(FLM)=0.1
‐0.25
0
0 0.25 0.5 0.75 1 1.25
P
Q=tanα *Pg ‐ (SCR‐NLM*cosθ)
•tanα =tanβ‐NLM[0.258]
•
cos
β
= 1/(1+FLM) [0 909
β
= 24 6⁰]
‐
1
‐0.75
Operating
Limits
Limits are reduced by:
0.75
1
Q
Limits
are
reduced
by:
•HighXd/LowSCR
•
Slow Exciter
0
0.25
0.5
P
Slow
Exciter
‐0.5
‐0.25
0
0 0.25 0.5 0.75 1 1.25
P
‐1
/ /
RatedMVA=200MVA
/
Xd=1.5
/
Ratedpowerfactor=0.9
220
180MW Generator/Slow-Acting Exciter
RATED MW
140
160
180
200
220
(
MW)
60
80
100
120
140
R
EAL POWER
(
0
20
40
60
-
100
21
GENERATORS
Case Study
/
/
RatedMVA=200MVA
/
Xd=1.5
/
Ratedpowerfactor=0.9
220
180MW Generator/Fast-Acting Exciter
RATED MW
140
160
180
200
220
(MW)
60
80
100
120
140
R
EAL POWER
0
20
40
-1
00
5
50
5
REACTIVE POWER (MVAR)
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