10 Stability
10 Stability
1 Network Stability
Electrical Network Stability Electrical Network Stability
APPS APPS
Summary
y Summary
y
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● An electrical energy network is a complex structure system, made of a ● An electrical energy network is a complex structure system, made of a
certain amount of production units, interconnected through transmission certain amount of production units, interconnected through transmission
and distribution grids and distribution grids
● This system is normally in a given equilibrium state: it is said in ● This system is normally in a given equilibrium state: it is said in
synchronous operation synchronous operation
● In particular
particular, fundamental equilibrium between production and ● In particular
particular, fundamental equilibrium between production and
consumption must be ensured in terms of : consumption must be ensured in terms of :
● ACTIVE POWER (linked to the network frequency) ● ACTIVE POWER (linked to the network frequency)
● REACTIVE POWER (linked to the network voltage map) ● REACTIVE POWER (linked to the network voltage map)
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Problematic: stabilityy issues Problematic: stabilityy issues
An electrical network in equilibrium state, i.e. in a given An electrical network in equilibrium state, i.e. in a given
steady state, is permanently subject to disturbances of any steady state, is permanently subject to disturbances of any
kind kind
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● Network parameters that can be affected (energy quality): ● Network parameters that can be affected (energy quality):
P Power P Power
U Voltage U Voltage
F Frequency F Frequency
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Problematic: stabilityy issues Problematic: stabilityy issues
● The basic questions to be answered by network stability studies are the ● The basic questions to be answered by network stability studies are the
following: following:
●what happens during a disturbance (voltage and frequency drift, ●what happens during a disturbance (voltage and frequency drift,
protections tripping, …)? protections tripping, …)?
●what will be the new operation point after
f the disturbance has ●what will be the new operation point after
f the disturbance has
disappear? disappear?
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●Synchronous
Synchronous operation ●Synchronous
Synchronous operation
A synchronous machine connected to other synchronous machines through A synchronous machine connected to other synchronous machines through
electrical network is said in synchronous operation with the rest of the electrical network is said in synchronous operation with the rest of the
network if its electrical speed is equal to the network’s
network s voltage frequency at network if its electrical speed is equal to the network’s
network s voltage frequency at
connection node, or to other machines’ electrical speed connection node, or to other machines’ electrical speed
An electric network is said in synchronous operation if all connected An electric network is said in synchronous operation if all connected
machines are in synchronous operation with the network and between machines are in synchronous operation with the network and between
together together
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Paul Bourotte’s ‘quintuplette’
q p ((1897)) Paul Bourotte’s ‘quintuplette’
q p ((1897))
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●Static stability,
stability or small-signal
small signal stability ●Static stability,
stability or small-signal
small signal stability
An electric network is said in static stability conditions if, after a small An electric network is said in static stability conditions if, after a small
disturbance, it reaches a new steady state very close to initial steady state disturbance, it reaches a new steady state very close to initial steady state
A smallll di
disturbance
t b iis a di
disturbance
t b ffor which
hi h lilinearization
i ti off th
the system’s
t ’ A smallll di
disturbance
t b iis a di
disturbance
t b ffor which
hi h lilinearization
i ti off th
the system’s
t ’
equations is still justified equations is still justified
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Definitions and terminology
gy Definitions and terminology
gy
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Transient Mid and long Large voltage Transient Mid and long Large voltage
stability terms stability disturbances stability terms stability disturbances
Large disturb.
disturb Large disturb.
disturb
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● Machine internal angle transient stability: ● Machine internal angle transient stability:
●large disturbances ●large disturbances
●fast dynamics (first aperiodical oscillations) ●fast dynamics (first aperiodical oscillations)
●typical study duration of few seconds ●typical study duration of few seconds
● Voltage
V lt transient
t i t stability
t bilit : ● Voltage
V lt transient
t i t stability
t bilit :
●large voltage disturbances ●large voltage disturbances
p , loads dynamics,
●events like operations, y , on load tap-changers,
p g , etc. p , loads dynamics,
●events like operations, y , on load tap-changers,
p g , etc.
●protections and control systems coordination ●protections and control systems coordination
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Static stability
y Static stabilityy
● Concerns small disturbances, for which electric parameters variations ● Concerns small disturbances, for which electric parameters variations
are slow and continuous. Linearization of network’s model equations is are slow and continuous. Linearization of network’s model equations is
then jjustified ((in p
particular,, the time variable does not occur)) then jjustified ((in p
particular,, the time variable does not occur))
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Loss of angle
g static stability
y Loss of angle
g static stability
y
t t
disturbance duration disturbance duration
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Loss of angle
g static stability
y Loss of angle
g static stability
y
t t
disturbance duration disturbance duration
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Conservation of angle
g static stability
y Conservation of angle
g static stability
y
● Damping and synchronizing torque coefficients are all positive ● Damping and synchronizing torque coefficients are all positive
● Internal angle is subjected to a damped oscillation and reaches a final ● Internal angle is subjected to a damped oscillation and reaches a final
value (generally different from initial value) that corresponds to a new value (generally different from initial value) that corresponds to a new
equilibrium equilibrium
t t
disturbance duration disturbance duration
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Introduction: Issues and definitions Introduction: Issues and definitions
Theoretical reminder Theoretical reminder
Regulators modeling Regulators modeling
Parameters affecting
g transmitted p
power Parameters affecting
g transmitted p
power
Risky situations Risky situations
Black-Outs Black-Outs
Studies
S ud es to
o be ca
carried
ed ou
out Studies
S ud es to
o be ca
carried
ed ou
out
Application: case studies Application: case studies
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Generator and rotating
g fields Generator and rotating
g fields
INDUCED INDUCED
(stator) (stator)
MAGNETIC MAGNETIC
FIELD FIELD
Driving
g and resistant torques
q Driving
g and resistant torques
q
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Rotating
g masses equation
q Rotating
g masses equation
q
● Acceleration or deceleration of the rotating masses is linked to the ● Acceleration or deceleration of the rotating masses is linked to the
difference between electrical torque (braking torque) and mechanical difference between electrical torque (braking torque) and mechanical
masses inertia constant J
torque (driving torque) through the rotating masses’ masses inertia constant J
torque (driving torque) through the rotating masses’
(kg.m²) (kg.m²)
Will the internal angle stabilize into a normal and Will the internal angle stabilize into a normal and
synchronous
h ti ?
operation? synchronous
h ti ?
operation?
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f / P coupling
p g f / P coupling
p g
● The fundamental rotating masses equation can be written as follows: ● The fundamental rotating masses equation can be written as follows:
J · (2/p)² · (f0 + f(t)) · ∂f/∂t = Pm(t) - Pe(t) J · (2/p)² · (f0 + f(t)) · ∂f/∂t = Pm(t) - Pe(t)
the proportionality relation is linked to the group the proportionality relation is linked to the group
‘turbine+generator’ construction (inertia, ...) ‘turbine+generator’ construction (inertia, ...)
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The link with internal angle
g The link with internal angle
g
Mechanical power delivered to the generator: Pm Mechanical power delivered to the generator: Pm
Electrical power delivered by the generator : Pe Electrical power delivered by the generator : Pe
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Equivalent
q diagram
g of a network Equivalent
q diagram
g of a network
generator
t t
transformer
f li
line i fi it network
infinite t k generator
t t
transformer
f li
line i fi it network
infinite t k
G G
G S L R G S L R
I I
Xd Xt Rt Xl Rl Xd Xt Rt Xl Rl
E VS VL VR E VS VL VR
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Equivalent
q diagram
g of a network Equivalent
q diagram
g of a network
G I R G I R
XT = Xd + Xt + Xl RT = Rt + Rl XT = Xd + Xt + Xl RT = Rt + Rl
E VR E VR
The mesh’ law is expressed as follows: E = VR + (RT + jXT) · I The mesh’ law is expressed as follows: E = VR + (RT + jXT) · I
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Kapp’s
pp diagram
g Kapp’s
pp diagram
g
E E
jXTI V jXTI V
VR RTI VR RTI
I I
V V
Neglecting RT beside XT, it results the following: Neglecting RT beside XT, it results the following:
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U / Q coupling
p g U / Q coupling
p g
● Transmission of definite active power P and reactive power Q between ● Transmission of definite active power P and reactive power Q between
two points of a network is accompanied by: two points of a network is accompanied by:
● an angular shift between the voltages E and VR ● an angular shift between the voltages E and VR
● a voltage drop: E - VR ≈ V ● a voltage drop: E - VR ≈ V
● The difference between E and VR voltages’ magnitudes (being close to ● The difference between E and VR voltages’ magnitudes (being close to
V) is mainly due reactive power transmission from G towards R V) is mainly due reactive power transmission from G towards R
g drop
To reduce the voltage p V,, one must g drop
To reduce the voltage p V,, one must
then avoid to carry reactive energy, and then avoid to carry reactive energy, and
therefore try to produce it at the nearest therefore try to produce it at the nearest
from
f consumption
ti places
l from
f consumption
ti places
l
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Transmittable p
powers Transmittable p
powers
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pp
Apparent p
power transmitted pp
Apparent p
power transmitted
G I R G I R
jXTI jXTI
ZT = RT + jXT ZT = RT + jXT
E VR RTI E VR RTI
The apparent power transmitted to infinite network (node R) is: The apparent power transmitted to infinite network (node R) is:
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Transmittable active power
p Transmittable active power
p
If the network resistance is neglected beside its reactance (RT << XT): If the network resistance is neglected beside its reactance (RT << XT):
● ZT = jXT ● ZT = jXT
● = /2 ● = /2
then the active power transmitted to the infinite network (node R) is: then the active power transmitted to the infinite network (node R) is:
Transmittable active p
power Transmittable active p
power
G S L R G S L R
I I
Xd Xt Rt Xl Rl Xd Xt Rt Xl Rl
E VS VL VR E VS VL VR
If instead of fix E (constant excitation), one fixes VS (voltage regulation), If instead of fix E (constant excitation), one fixes VS (voltage regulation),
then the maximal transmitted active power from S towards R becomes: then the maximal transmitted active power from S towards R becomes:
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Transmittable active p
power Transmittable active p
power
G S L R G S L R
I I
Xd Xt Rt Xl Rl Xd Xt Rt Xl Rl
E VS VL VR E VS VL VR
P’’max = (VR · VL) / Xl > P’max > Pmax P’’max = (VR · VL) / Xl > P’max > Pmax
Voltage regulators action (excitation systems) allows then stable operation of the machine Voltage regulators action (excitation systems) allows then stable operation of the machine
in a zone where it is not « naturally » stable in a zone where it is not « naturally » stable
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0 0 /2
/2 ’0 0 0 /2
/2 ’0
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Areas equality
q y theorem Areas equality
q y theorem
b final situation: Pméca = Pm1 b final situation: Pméca = Pm1
a initial situation: Pméca = Pm0 a initial situation: Pméca = Pm0
-> new equilibrium point: = 1 -> new equilibrium point: = 1
0 0 1 /2 m
/2 L 0 0 1 /2 m
/2 L
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Behn-Eschenburg
g Diagram
g Behn-Eschenburg
g Diagram
g
Operating
p gppoint Operating
p gppoint
S S
P I P I
Magnitude of E given Magnitude of E given
excitation Xd excitation Xd
E ZR E ZR
VS VS
Internal angle
of the machine
E Internal angle
of the machine
E
jXdI jXdI
Q Q
VS VS
I P = (E · VS · sin) / Xd I P = (E · VS · sin) / Xd
Q = (E · VS · cos - VS²)/ Xd Q = (E · VS · cos - VS²)/ Xd
Current fixed by Current fixed by
the load Voltage fixed by the network the load Voltage fixed by the network
(nominal voltage of the machine) (nominal voltage of the machine)
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p g limits: active p
Operating power p g limits: active p
Operating power
E E
jXdI jXdI
Q Q
VS VS
I I
Motor operation Motor operation
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Operating
p g limits: apparent
pp power
p Operating
p g limits: apparent
pp power
p
E E
jXdI jXdI
Q Q
VS VS
I I
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Loss of Loss of
excitation limit excitation limit
E E
jXdI jXdI
Q Q
VS VS
I I
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Operating
p g limits: internal angle
g Operating
p g limits: internal angle
g
E E
jXdI jXdI
I I
Q Q
VS VS
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Operating
p g limits: conclusion Operating
p g limits: conclusion
S S
P P
I I
Xd Xd
E ZR E ZR
VS VS
E E
jXdI jXdI
Q Q
VS VS
I I
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Primary and secondary Primary and secondary
voltage / reactive power control voltage / reactive power control
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Voltage:
g a fluctuating
g value Voltage:
g a fluctuating
g value
Need for a ‘continuous’ watch of the voltage on transmission and Need for a ‘continuous’ watch of the voltage on transmission and
distribution grids distribution grids
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Voltage
g control and static stability
y Voltage
g control and static stability
y
PR, QR PR, QR
Assumptions: Assumptions:
I I
● E = constant as PR changes (constant excitation) ● E = constant as PR changes (constant excitation)
X ● QR = 0 (reactive power compensation at X ● QR = 0 (reactive power compensation at
E ZR transformation stations)) E ZR transformation stations))
VR VR
● VR not regulated ● VR not regulated
It results VR = E · cos, i.e.: (PR = VR² · sin2) / 2X It results VR = E · cos, i.e.: (PR = VR² · sin2) / 2X
The maximal transmittable power per phase is therefore PMax = VR² / 2X The maximal transmittable power per phase is therefore PMax = VR² / 2X
If VR is maintained equal to E by reactive compensation (QR ≠ 0), then: If VR is maintained equal to E by reactive compensation (QR ≠ 0), then:
P
P’Max = E · VR /X ≈ E²
E / X > PMax P
P’Max = E · VR /X ≈ E
E² / X > PMax
Voltage control on several nodes of the network permits to improve its Voltage control on several nodes of the network permits to improve its
static stability static stability
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Voltage
g control and static stability
y Voltage
g control and static stability
y
E² E4 E² cos = 1 E² E4 E² cos = 1
VR ² QR X X PR ² QR VR ² QR X X PR ² QR
2 4 X² X cos = 0.95 2 4 X² X cos = 0.95
cos = 0.9 cos = 0.9
Q = -0.2 p.u. Q = -0.2 p.u.
(compensation) (compensation)
1 PR / PMax 1 PR / PMax
VR ² X PMax QR PMax ² PR ² 2PMax QR
VR ² X PMax QR PMax ² PR ² 2PMax QR
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Primary
y control Primaryy control
Local, fast, and continuous stator voltage control Local, fast, and continuous stator voltage control
measure measure
Vs Vs
Vref + Vs Vref + Vs
-
AVR G -
AVR G
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Secondary
y control Secondaryy control
Regional and continuous network voltage control Regional and continuous network voltage control
measure measure
Vs Vs
Vref + Vs Vref + Vs
-
AVR G -
AVR G
+ Q + Q
V V
Vp Vp
Q control Q control
Qlim Qlim
N - N -
PI PI
+ +
other controlling
gggroups
p Vpref other controlling
gggroups
p Vpref
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●In the case of balance rupture between production and ●In the case of balance rupture between production and
consumption, frequency is the first parameter that reflects consumption, frequency is the first parameter that reflects
the evolution the evolution
●The risks if frequency is not controlled: ●The risks if frequency is not controlled:
● Loss of synchronism ● Loss of synchronism
● Electrical and mechanical constraints applied on equipments sensitive to ● Electrical and mechanical constraints applied on equipments sensitive to
frequency (turbine blades, windings, etc.) frequency (turbine blades, windings, etc.)
● Generator stall, leading to Blackout in extreme cases ● Generator stall, leading to Blackout in extreme cases
oss o
● Loss of e
exploitation
p o a o du during
g reconstruction
eco s uc o p phase
ase oss o
● Loss of e
exploitation
p o a o du during
g reconstruction
eco s uc o p phase
ase
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Droop
p Droop
p
The droop defines the relation between active power and frequency of a The droop defines the relation between active power and frequency of a
machine or a production plant machine or a production plant
fmin fmin
P P
P1 P0 P1 Pn P1 P0 P1 Pn
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The energy that is necessary to maintain frequency is proportional to The energy that is necessary to maintain frequency is proportional to
produced power, the proportionality coefficient is called inertia constant produced power, the proportionality coefficient is called inertia constant
(H in MW
(H, MW.s-1
s-1 / MVA) (H in MW
(H, MW.s-1
s-1 / MVA)
f f
fmax fmax
● This energy is called ● This energy is called
f1 f1
composite frequency response composite frequency response
f0 f0
f1
characteristic f1
characteristic
● = Pn / (R · f0), in MW / Hz ● = Pn / (R · f0), in MW / Hz
fmin ● The frequency variation rate fmin ● The frequency variation rate
depends on the electrical depends on the electrical
system inertia constant system inertia constant
P P
P1 P0 P1 Pn P1 P0 P1 Pn
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Primary
y control Primaryy control
Local, fast, and continuous active power control Local, fast, and continuous active power control
1/R 1/R
P f P f
Pref + Pref +
-
Regul. T G -
Regul. T G
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Secondary
y control Secondaryy control
Regional and continuous frequency control Regional and continuous frequency control
interconnection line interconnection line
1/R 1/R
P P
Pref + f Pref + f
-
Regul. T G -
Regul. T G
+ +
P PI P PI
Ps f Ps f
X secondary reserve
f0 X secondary reserve
f0
PIref PIref
N + N +
- -
PI + PI +
- -
other controlling groups other controlling groups
= secondary composite = secondary composite
frequency response frequency response
● At national level characteristic (MW/Hz) ● At national level characteristic (MW/Hz)
● Constant frequency and maintain of power exchanges on interconnection ● Constant frequency and maintain of power exchanges on interconnection
li
lines att th
their
i contractual
t t l values
l li
lines att th
their
i contractual
t t l values
l
● Response time: few minutes ● Response time: few minutes
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Conclusion on f / P control Conclusion on f / P control
● Primary control realizes production / consumption balance and ● Primary control realizes production / consumption balance and
stabilizes the network stabilizes the network
● Leads to a slow frequency and inter-regional
inter regional power exchange drift ● Leads to a slow frequency and inter-regional
inter regional power exchange drift
(interconnections) (interconnections)
f f
f1 f1
● fast action of primary control ● fast action of primary control
f0 f0
P P
P1 P0 Pn P1 P0 Pn
● Secondary control regulates frequency and inter-regional exchanges ● Secondary control regulates frequency and inter-regional exchanges
● Re-dispatching of primary control set points ● Re-dispatching of primary control set points
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R
Regulators
l t modeling
d li R
Regulators
l t modeling
d li
Parameters affecting
g transmitted p
power Parameters affecting
g transmitted p
power
Risky situations Risky situations
Black-Outs Black-Outs
Studies
S ud es to
o be ca
carried
ed ou
out Studies
S ud es to
o be ca
carried
ed ou
out
Application: case studies Application: case studies
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Objectives
j of modeling
g Objectives
j of modeling
g
● A model is a mathematic image (state matrix, differential equations, ● A model is a mathematic image (state matrix, differential equations,
etc.) of a given system that aims to represent in a more or less detailed etc.) of a given system that aims to represent in a more or less detailed
way the real physical behavior of the system way the real physical behavior of the system
● The goal of a mathematical modeling of a physical system is to ● The goal of a mathematical modeling of a physical system is to
determine the system behavior (machine, or more generally electric determine the system behavior (machine, or more generally electric
system) facing a given disturbance system) facing a given disturbance
● Electrical network dynamic simulation software are available, such as: ● Electrical network dynamic simulation software are available, such as:
● PSAF/STAB CYME (Canada) ● PSAF/STAB CYME (Canada)
● EUROSTAG RTE (France) / TRACTEBEL (Beglium) ● EUROSTAG RTE (France) / TRACTEBEL (Beglium)
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From p
physics
y to mathematic model From p
physics
y to mathematic model
voltage
g regulation
g voltage
g regulation
g
control command controlled control command controlled
measured set point measured set point
signal signal value signal signal value
values values
Vref Vref
+ +
Vs Vc Vr Efd Vs Vc Vr Efd
Is transducer -
AVR + exciter generator Vs Is transducer -
AVR + exciter generator Vs
- - - -
saturation saturation
stabilization stabilization
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From p
physics
y to mathematic model From p
physics
y to mathematic model
speed
p /p g
power regulation speed
p /p g
power regulation
set point command controlled set point command controlled
measured measured
control g
signal value control g
signal value
value value
signal signal
Ωref Ωref
+
admission
d i i +
admission
d i i
m m
Ω
-
servo-pilot prime mover generator Pe Ω
-
servo-pilot prime mover generator Pe
- transmission - transmission
stabilization stabilization
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Voltage
g regulation:
g yp
typical model Voltage
g regulation:
g yp
typical model
Ω0 Ω0
Power System Stabilizer Power System Stabilizer
VSmax VSmax
1+T1s Tss + 1+T1s Tss +
Ks Ω Ks Ω
1+T2s 1+Tss - 1+T2s 1+Tss -
VSmin VSmin
Vref Vref
transducer transducer
g Regulator
Automatic Voltage g exciter g Regulator
Automatic Voltage g exciter
Vs VRmax Vs VRmax
Is Rc+jXc Is Rc+jXc
+ + + + + +
Vc + 1+TCs KA Vr 1 Vc + 1+TCs KA Vr 1
Vs Efd Vs Efd
+ - - 1+TBs 1+TAs + - TEs + - - 1+TBs 1+TAs + - TEs
Vf VUEL VRmin Vf VUEL VRmin
+ +
Ke Ke
+ +
X Ae·eBex X Ae·eBex
stabilization stabilization
saturation saturation
KFs KFs
1+TFs 1+TFs
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p
Speed g
regulation: hydraulic
y p
Speed g
regulation: hydraulic
y
servo-pilot servo-pilot
Ω0 Ω0
Tmax-Ouv 1 Tmax-Ouv 1
gate turbine gate turbine
+ +
KS 1 1 F 1-TWs KS 1 1 F 1-TWs
Ω - m Ω - m
- 1+TPs s 1+TGs 1+0.5·TWs - 1+TPs s 1+TGs 1+0.5·TWs
Tmax-Ferm 0 Tmax-Ferm 0
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Speed
p g
regulation: thermal Speed
p g
regulation: thermal
servo-pilot Ω0 servo-pilot Ω0
1 1
Tmax-Ouv Kpr Tmax-Ouv Kpr
1 + + 1 + +
KSM
+ +
Kg Ω KSM
+ +
Kg Ω
s - - - s - - -
1 - 1 -
Tmax-Ferm Tmax-Ferm
0 Tis 0 Tis
turbine turbine
+ + + +
+ + + +
admission K K admission K K
1 1 + 1 1 +
Pref Pt Fhp 1 + Pref Pt Fhp 1 +
X boiler X m X boiler X m
+ - 1+Tchs 1+Ts 1+Ts + + - 1+Tchs 1+Ts 1+Ts +
Kpd x² K K Kpd x² K K
+ + + +
+ + + +
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1+TCs x KA Vr 1+TCs x KA Vr
1+TBs 1+TAs 1+TBs 1+TAs
VUEL VRmin VUEL VRmin
1 TCs
1+T dx 1 T dε 1 1 TCs
1+T dx 1 T dε 1
l d l fil
lead-lag filter: x C ε llead-lag
d l fil
filter: x C ε
1+TBs dt TB TB dt TC 1+TBs dt TB TB dt TC
KA dVr 1 K KA dVr 1 K
simple-lag filter: Vr A x simple-lag filter: Vr A x
1+TAs dt TA TA 1+TAs dt TA TA
d² Vr TA TB dVr 1 K T dε 1 d² Vr TA TB dVr 1 K T dε 1
Vr A C ε Vr A C ε
dt ² TA TB dt TA TB TA T
B dt TC dt ² TA TB dt TA TB TA T
B dt TC
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Transfer function Transfer function
Automatic Voltage Regulator Automatic Voltage Regulator
VRmax VRmax
Vr(s) 1 Tc s Vr(s) 1 Tc s
Laplace transformation: H(s) K A Laplace transformation: H(s) K A
ε(s) (1 TB s) (1 TA s) ε(s) (1 TB s) (1 TA s)
The transfer function poles (spi so as the denominator is equal to zero) provide The transfer function poles (spi so as the denominator is equal to zero) provide
indication about the system stability (Eigen modes): indication about the system stability (Eigen modes):
●real part: damping (negative real part stable mode) ●real part: damping (negative real part stable mode)
●imaginary part: frequency of oscillation ●imaginary part: frequency of oscillation
The transfer function zeros (s0i so as the numerator is equal to zero) provide The transfer function zeros (s0i so as the numerator is equal to zero) provide
indication about the system robustness (overreach, etc.) indication about the system robustness (overreach, etc.)
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Parameters affecting
g transmitted p
power Parameters affecting
g transmitted p
power
Risky situations Risky situations
Black-Outs Black-Outs
S ud es to
Studies o be ca ed ou
carried out S ud es to
Studies o be ca ed ou
carried out
Application: case studies Application: case studies
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Machine p g
parameters: internal angle Machine p g
parameters: internal angle
Pm Pm
Pe Pe
PMax PMax
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Machine parameters:
p internal angle
g Machine p
parameters: internal angle
g
Pm Pm
Pe Pe
PMax PMax
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Machine p g
parameters: internal angle Machine p g
parameters: internal angle
Pm Pm
Pe Pe
PMax PMax
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Machine parameters:
p excitation Machine parameters:
p excitation
Pm Pm
E E
Pe Pe
Nominal excitation Nominal excitation
PMax PMax
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Machine p
parameters: excitation Machine p
parameters: excitation
Pm Pm
E E
Pe Pe
Over-Excitation Over-Excitation
PMax PMax
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Machine p
parameters: excitation p
Machine parameters: excitation
Pm Pm
E E
Pe Pe
Under-Excitation Under-Excitation
PMax PMax
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Network parameters: Network parameters:
network
impedance of the link to infinite net ork network
impedance of the link to infinite net ork
Pm Pm
G G
Pe Pe
dense meshed grid dense meshed grid
PMax PMax
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Pm Pm
G G
Pe Pe
light meshed grid light meshed grid
PMax PMax
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Network p g
parameters: network voltage Network p g
parameters: network voltage
Pm Pm
VR VR
Pe Pe
The influence of the network voltage on The influence of the network voltage on
the transmittable active power is analogue the transmittable active power is analogue
PMax PMax
the influence of excitation voltage the influence of excitation voltage
Pm Pm
PMax PMax
Pe Pe
e e
0 /2
/ 0 /2
/
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Line opening
p g Line opening
p g
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p 1: stability
Example y is conserved p 1: stability
Example y is conserved
Pm Pm
G G
Pe Pe
initial state initial state
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Example
p 1: stability
y is conserved Example
p 1: stability
y is conserved
Pm Pm
G G
Pe Pe
line opening line opening
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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p 1: stability
Example y is conserved p 1: stability
Example y is conserved
Pm Pm
G G
Pe Pe
acceleration phase acceleration phase
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Example
p 1: stability
y is conserved Example
p 1: stability
y is conserved
Pm Pm
G G
Pe Pe
braking phase braking phase
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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p 1: stability
Example y is conserved p 1: stability
Example y is conserved
Pm Pm
G G
Pe Pe
stabilization stabilization
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Example
p 2: stability
y is lost Example
p 2: stability
y is lost
Pm Pm
G G
Pe Pe
initial state initial state
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
Schneider Electric - Energy Automation – Technical Institute 85 Schneider Electric - Energy Automation – Technical Institute 85
p 2: stability
Example y is lost p 2: stability
Example y is lost
Pm Pm
G G
Pe Pe
line opening line opening
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Example
p 2: stability
y is lost Example
p 2: stability
y is lost
Pm Pm
G G
Pe Pe
acceleration phase acceleration phase
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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p 2: stability
Example y is lost p 2: stability
Example y is lost
Pm Pm
G G
Pe Pe
stalling stalling
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Global voltage
g drop
p Global voltage
g drop
p
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g drop
Voltage p g drop
Voltage p
Pm Pm
VR VR
Pe Pe
initial state initial state
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Voltage
g drop
p Voltage
g drop
p
Pm Pm
VR VR
Pe Pe
network voltage drop network voltage drop
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Voltage
g drop
p Voltage
g drop
p
Pm Pm
VR VR
Pe Pe
acceleration phase acceleration phase
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Voltage
g drop
p Voltage
g drop
p
Pm Pm
VR VR
Pe Pe
voltage is back voltage is back
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
Schneider Electric - Energy Automation – Technical Institute 93 Schneider Electric - Energy Automation – Technical Institute 93
Voltage
g drop
p Voltage
g drop
p
Pm Pm
VR VR
Pe Pe
braking phase braking phase
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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p of U
Influence of the depth p of U
Influence of the depth
VR VR VR VR
Pm Vn Pm Vn Pm Vn Pm Vn
PMax PMax PMax PMax
Pm Pm Pm Pm
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VR VR VR VR
Pm Vn Pm Vn Pm Vn Pm Vn
PMax PMax PMax PMax
Pm Pm Pm Pm
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Short-circuit on the network Short-circuit on the network
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Short-circuit Short-circuit
Pm Pm
G G
Pe Pe
initial state initial state
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Short-circuit Short-circuit
Pm Pm
G G
Pe Pe
occurrence of a short-circuit occurrence of a short-circuit
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Short-circuit Short-circuit
Pm Pm
G G
Pe Pe
acceleration phase acceleration phase
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Short-circuit Short-circuit
Pm Pm
G G
Pe Pe
line tripping line tripping
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Short-circuit Short-circuit
Pm Pm
G G
Pe Pe
braking phase braking phase
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Influence of the type
yp of short-circuit Influence of the type
yp of short-circuit
Pm Pm
no short-circuit no short-circuit
0 /2
/2 0 /2
/2
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G G G G
Pm Pm Pm Pm
PMax
M PMax
M PMax
M PMax
M
Pm Pm Pm Pm
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Influence of fault clearing
g time Influence of fault clearing
g time
G G G G
t t t t
Pm Pm Pm Pm
PMax PMax PMax PMax
Pm Pm Pm Pm
0 /2 0 /2
/ 0 /2 0 /2
/
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Automatic recloser Automatic recloser
Pm Pm
G G
Pe Pe
initial state initial state
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
Schneider Electric - Energy Automation – Technical Institute 107 Schneider Electric - Energy Automation – Technical Institute 107
Pm Pm
G G
Pe Pe
short-circuit short-circuit
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Automatic recloser Automatic recloser
Pm Pm
G G
Pe Pe
trip trip
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Pm Pm
G G
Pe Pe
reclosing reclosing
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Synchro-check
y Synchro-check
y
● The generator and the network are synchronous together ● The generator and the network are synchronous together
G G
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Synchro-check
y Synchro-check
y
● Short-circuit: the link between the generator and the network is very ● Short-circuit: the link between the generator and the network is very
weak weak
G G
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Synchro-check
y Synchro-check
y
● Line opening: the generator evolves independently from the network ● Line opening: the generator evolves independently from the network
G G
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Synchro-check
y Synchro-check
y
● Reclosing: it is essential to check the synchronism between generator ● Reclosing: it is essential to check the synchronism between generator
and network voltage before allowing line reclosing and network voltage before allowing line reclosing
G G
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Synchro-check
y Synchro-check
y
G G
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Synchro-check
y Synchro-check
y
G G
synchronism conditions not OK: wait synchronism conditions not OK: wait
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Synchro-check
y Synchro-check
y
G G
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Heavy
y load switched on Heavy
y load switched on
Pm Pm
G G
Pe Pe
initial state initial state
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Pm Pm
G G
Pe Pe
load switch-on load switch-on
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Heavy
y load switched on Heavy
y load switched on
Pm Pm
G G
Pe Pe
primary control (droop) primary control (droop)
PMax PMax
Pm Pm
PMax PMax
Pm Pm
e e
0 /2
/ 0 /2
/
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Bl k O t
Black-Outs Bl k O t
Black-Outs
S ud es to
Studies o be ca ed ou
carried out S ud es to
Studies o be ca ed ou
carried out
Application: case studies Application: case studies
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What is a black-out ? What is a black-out ?
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Major
j incident formation mechanism Major
j incident formation mechanism
initiating
g critical Black initiating
g critical Black
event event Out event event Out
normal pre- quasi-steady state normal normal pre- quasi-steady state normal
series reconstruction series reconstruction
situation
s tuat o incident
c de t evolution
e o ut o situation ssituation
tuat o incident
c de t evolution
e o ut o situation
● Pre-conditions ● Pre-conditions
● Stressed system: summer or winter consumption peaks, N-1 criterion ● Stressed system: summer or winter consumption peaks, N-1 criterion
● Inappropriate reactive power spinning reserve ● Inappropriate reactive power spinning reserve
● Some major equipments out of service ● Some major equipments out of service
● Aging equipments ● Aging equipments
● Natural causes: wind, storms, geomagnetic disturbances, fires, etc. ● Natural causes: wind, storms, geomagnetic disturbances, fires, etc.
● Initiating events and aggravating factors ● Initiating events and aggravating factors
● Natural causes: storm, geomagnetic storm, earthquake, lightning strike, ● Natural causes: storm, geomagnetic storm, earthquake, lightning strike,
contact with a tree,… contact with a tree,…
● Technical
T h i l causes: short-circuits,
h t i it componentt failures,
f il heavy
h lload,
d major
j ● Technical
T h i l causes: short-circuits,
h t i it componentt failures,
f il heavy
h lload,
d major
j
component maintenance,… component maintenance,…
● Human causes: maneuver errors, wrong or inappropriate communications ● Human causes: maneuver errors, wrong or inappropriate communications
between operators, lack of training,… between operators, lack of training,…
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SLOVENIA SLOVENIA
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Defense plan
p Defense plan
p
‘N-k’ rule emergency production units ‘N-k’ rule emergency production units
management islanding management islanding
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Defense p
plan Defense p
plan
...to avoid incidents propagation and to plan ...to avoid incidents propagation and to plan
network reconstruction network reconstruction
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Reconstruction plan
p Reconstruction plan
p
successful successful
islanding islanding
Reconstruction plan
p Reconstruction plan
p
● DC links (HVDC) to stop disturbances propagation ● DC links (HVDC) to stop disturbances propagation
● PMU (Phasor
(Ph M
Measurement U
Units)
i ) iinstallation:
ll i ● PMU (Phasor
(Ph M
Measurement U
Units)
i ) iinstallation:
ll i
WAMS / WACS (Wide Area Measurement / Control System) WAMS / WACS (Wide Area Measurement / Control System)
● FACTS (flexible AC transmission system) for a better control of power ● FACTS (flexible AC transmission system) for a better control of power
fluxes fluxes
● System reconfiguration into energetically independant islands – cells ● System reconfiguration into energetically independant islands – cells
g
and distributed intelligence concepts
p g
and distributed intelligence concepts
p
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HV transmission network stabilityy studies HV transmission network stabilityy studies
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sub-synchronous
b h ffrequencies
i sub-synchronous
b h ffrequencies
i
● Low frequency active power exchanges between generators or between ● Low frequency active power exchanges between generators or between
areas : areas :
inter-area inter-area
local modes local modes
modes modes
0.1
0 1 Hz 0.8
0 8HHz 0.1
0 1 Hz 0.8
0 8HHz
~ 0.7 Hz ~ 2.5 Hz ~ 0.7 Hz ~ 2.5 Hz
● Power System Stabilizer (PSS): regulation loop aiming to damp these ● Power System Stabilizer (PSS): regulation loop aiming to damp these
oscillations oscillations
Schneider Electric - Energy Automation – Technical Institute 137 Schneider Electric - Energy Automation – Technical Institute 137
● Small-signal stability to determine des oscillanting modes that are naturally ● Small-signal stability to determine des oscillanting modes that are naturally
sustained (frequency and damping): sustained (frequency and damping):
● Determine PSS and AVR settings to damp the most problematic modes ● Determine PSS and AVR settings to damp the most problematic modes
Schneider Electric - Energy Automation – Technical Institute 138 Schneider Electric - Energy Automation – Technical Institute 138
Sub-synchronous
y frequencies
q Sub-synchronous
y frequencies
q
● Sustained shaft oscillations situations which appear spontaneously after ● Sustained shaft oscillations situations which appear spontaneously after
non-linearities: non-linearities:
●magnetic
magnetic circuit saturations ●magnetic
magnetic circuit saturations
●regulator limitations ●regulator limitations
●discrete events ●discrete events
● Resonance frequencies linked to electromechanical coupling between ● Resonance frequencies linked to electromechanical coupling between
machines and HV line series compensations machines and HV line series compensations
G G
5 Hz ~ 40-50 Hz 5 Hz ~ 40-50 Hz
● Sub-synchronous
Sub synchronous resonance analysis through dynamic simulation and ● Sub-synchronous
Sub synchronous resonance analysis through dynamic simulation and
small-signal study small-signal study
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Any HV network complexity increase will potentially lead to the Any HV network complexity increase will potentially lead to the
apparition of new oscillation modes. apparition of new oscillation modes.
● Analysis of induced disturbance through dynamic simulation and small- ● Analysis of induced disturbance through dynamic simulation and small-
signal
i l study
t d signal
i l study
t d
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Production units stabilityy studies Production units stabilityy studies
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What kind of study should be carried out What kind of study should be carried out
for unit
nit connection? for unit
nit connection?
Response to sudden events Response to sudden events
short-circuits; voltage drops; loss of load / production short-circuits; voltage drops; loss of load / production
CAPABILITY TO CONSERVE SYNCHRONISME / RISK OF MIS-COUPLING CAPABILITY TO CONSERVE SYNCHRONISME / RISK OF MIS-COUPLING
Oscillation modes study (Eigen modes / inter-area modes) Oscillation modes study (Eigen modes / inter-area modes)
power swings; resonances power swings; resonances
DAMPING OF LOW FREQUENCY OSCILLATIONS DAMPING OF LOW FREQUENCY OSCILLATIONS
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Connection to transmission network Connection to transmission network
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● ISLANDING ● ISLANDING
Th production
The d ti unitit mustt be
b able
bl to
t operate
t on its
it auxiliaries
ili i andd tto ensure Th production
The d ti unitit mustt be
b able
bl to
t operate
t on its
it auxiliaries
ili i andd tto ensure
voltage return on the network voltage return on the network
>>> The unit have to support the transmission network >>> The unit have to support the transmission network
Schneider Electric - Energy Automation – Technical Institute 144 Schneider Electric - Energy Automation – Technical Institute 144
Connection to distribution network Connection to distribution network
If not, the unit must disconnect from the grid in case of disturbance on the If not, the unit must disconnect from the grid in case of disturbance on the
distribution network distribution network
● ISLANDING ● ISLANDING
The owner may y carryy out a dynamic
y stabilityy studyy if he wishes to island The owner mayy carryy out a dynamic
y stabilityy studyy if he wishes to island
after a disconnection after a disconnection
>>> The
Th unitit mustt nott disturb
di t b the
th di
distribution
t ib ti network
t k >>> The
Th unitit mustt nott disturb
di t b the
th di
distribution
t ib ti network
t k
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Stability studies for Oil&Gas type Stability studies for Oil&Gas type
industries industries
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Why
y a stabilityy studyy for MV motors? Whyy a stabilityy studyy for MV motors?
start / re-acceleration start / re-acceleration
capability capability
~ ~
~ ~ ~ ~
~ ~
i d ti motors
induction t t
torque & currentt curves i d ti motors
induction t ttorque & currentt curves
Voltage Voltage
Speed Speed
I / In / n I / In / n
time time
1 1 1 1
0 N / Nsynchro 1 0 N / Nsynchro 1
Torque Torque
A deep voltage drop can lead to A deep voltage drop can lead to
motor stall Current motor stall Current
time time
Schneider Electric - Energy Automation – Technical Institute 148 Schneider Electric - Energy Automation – Technical Institute 148
Source change-over
g Source change-over
g
● Automatic change-over operation induce motors slow-down during the ● Automatic change-over operation induce motors slow-down during the
change-over, followed by a load increase for the new source change-over, followed by a load increase for the new source
A
Voltage A
Voltage
B B
DA DB DA DB
Speed Speed
DC DC
M M M M M M M M M M
Schneider Electric - Energy Automation – Technical Institute 149 Schneider Electric - Energy Automation – Technical Institute 149
Source change-over
g Source change-over
g
● If the voltage drop is too deep, the driving torque decreases... ● If the voltage drop is too deep, the driving torque decreases...
V lt
Voltage V lt
Voltage
Voltage Voltage
Torque Torque
Torque Torque
● ...motors don
don’tt re
re-accelerate
accelerate ● ...motors don
don’tt re
re-accelerate
accelerate
>>> load-shedding plan / fast load-shedding >>> load-shedding plan / fast load-shedding
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Short-circuit / voltage
g drop
p Short-circuit / voltage
g drop
p
● Voltage drop motors loose driving force ● Voltage drop motors loose driving force
● Short-circuit
Sh i i motors braking
b ki ● Short-circuit
Sh i i motors braking
b ki
● induction motors may stall if acceleration torque is too low ● induction motors may stall if acceleration torque is too low
● synchronous motors may loose synchronism if the disturbance goes on ● synchronous motors may loose synchronism if the disturbance goes on
for too long for too long
>>> p
protection p
plan validation / study
y >>> p
protection p
plan validation / study
y
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Schneider Electric - Energy Automation – Technical Institute 152 Schneider Electric - Energy Automation – Technical Institute 152
Static stability: Static stability:
theoretical study theoretical study
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Steady
y state calculation Steadyy state calculation
A A
Transmittable powers Transmittable powers
PnA = 15000 MW VA = 415 kV PnA = 15000 MW VA = 415 kV
GA PmaxAR = .3000 MW. MW GA PmaxAR = .3000 MW. MW
RA = 7.5 % A = .5.51° . RA = 7.5 % A = .5.51° .
PmaxBR = .2400 MW. MW PmaxBR = .2400 MW. MW
PchA = 9000 MW PchA = 9000 MW
PmaxAB = .3800 MW. MW PmaxAB = .3800 MW. MW
PgA = .10815 MW
. MW PgA = .10815 MW
. MW
R R
PiR = .461 MW. MW PiR = .461 MW. MW
PnB = 12000 MW PnB = 12000 MW
RB = 8 % RB = 8 %
f = 50 Hz f = 50 Hz
R R
PnB = 12000 MW
PiR = .-2839 . MW
2839 MW PnB = 12000 MW
PiR = .-2839 . MW
2839 MW
RB = 8 % RB = 8 %
B = .3000 .MW/Hz
MW/Hz B = .3000 .MW/Hz
MW/Hz
f = .50.1 Hz
. Hz f = .50.1 Hz
. Hz
B B
PchB = 13000 MW PchB = 13000 MW
PgB = .10424 MW
. MW PgB = .10424 MW
. MW
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14.4 MW steam turbine connection to 20 kV public 14.4 MW steam turbine connection to 20 kV public
distribution network distribution network
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Installation single-line
g diagram
g Installation single-line
g diagram
g
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Regulation
g models Regulation
g models
Th turbine
The t bi and
d its
it speed
d regulation
l ti Th turbine
The t bi and
d its
it speed
d regulation
l ti
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Regulation
g models Regulation
g models
Exciter and AVR Exciter and AVR
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Dynamic
y simulation: short-circuit Dynamic
y simulation: short-circuit
820 ms 820 ms
830 ms 830 ms
2.100 s 2.100 s
Schneider Electric - Energy Automation – Technical Institute 160 Schneider Electric - Energy Automation – Technical Institute 160
Dynamic
y simulation: loss of the network Dynamic
y simulation: loss of the network
Schneider Electric - Energy Automation – Technical Institute 161 Schneider Electric - Energy Automation – Technical Institute 161
To improve
p yyour knowledge
g ... To improve
p yyour knowledge
g ...
P. Kundur : « Power System Stability and P. Kundur : « Power System Stability and
Control », McGraw-Hill, 1994 Control », McGraw-Hill, 1994
RTE : Mémento de la sûreté du système électrique, édition 2004 RTE : Mémento de la sûreté du système électrique, édition 2004
Techniques de l’Ingénieur
l Ingénieur : D4092 “Réseaux
Réseaux d’interconnexion
d interconnexion et de Techniques de l’Ingénieur
l Ingénieur : D4092 “Réseaux
Réseaux d’interconnexion
d interconnexion et de
transport : réglage et stabilité“ transport : réglage et stabilité“
Schneider Electric - Energy Automation – Technical Institute 162 Schneider Electric - Energy Automation – Technical Institute 162