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106 陳敬燁
Power System Stabilization Using Virtua
l Synchronous Generator With AlternatingMoment of Inertia
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synchronous generators(SGs)
! rotating inertia
"! #isturbancessu##en changes
in$ecting the %inetic
energy to the &owergri#
SoSystemis robust againstinstability
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VI'UA S*+,-'.+.US G/+/'A.' S'U,U'/
swing e0uation :
its out&ut &ower an#
fre0uency are calculate#!
Measuring the 1oltage
an# currentsignals2
** J together with D determines the timeconstant
H bigger time constant, slowerresponse , smaller fre0uency #e1iation(aftera change or #isturbance)
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3A+G43A+G ,.+'. S'A/G* .5 A/'+AI+G I+/'IA
.ne cycle of the oscillation consists of four segments
** select a large 1alue of J #uring acceleration &hases to reduce the acceleration** select a small 1alue of J during deceleration phases to boost the deceleration.
he transients are su&&resse#
an#ω equals zero at the newequilibrium point
.scillation will sto&
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5i6e# 7 Alternating 7
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88fi6e# J cannot stabilize the fre0uency
When changing toalternating inertia
control
!stabilize the system"!su&&resses the fre0uency an# &ower oscillations
effecti1ely!
9am&ing factor! An ina&&ro&riate 1alue of #am&ing factor may result in a high
magnitu#e of oscillation or a sluggish res&onse"! -ere2 choosing #am&ing factor : ;
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9am&ing factor
! An ina&&ro&riate 1alue of #am&ing factor may result in a high magnitu#e of oscillation or a sluggish res&onse
"! -ere2 choosing #am&ing factor : ;
We can see the system o&eratesstably 2 an# the oscillations areeliminate# by the alternating
inertia i#ea
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SA3II* ASS/SSM/+ 3* /+/'G* 5U+,I.+ A+A*SIS
ω 0 J [−
P in(δ−
δ 1 ) + b( cos δ−
cos δ 1 ) ]
Ek , is the kinetic energy
EP is the potential energy
From Fig.4 start at point a
a to b
ω is zero and ! " is ma#imum&resum&tion of J $ % is needed.
Ek & % EP is ma#imum Ek is increasing, and Ep isdecreasing as ω increasesan# !" decreases
b to c ω decreases and ! " increasesthe total energy has #ecrease#
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89am&ing effecthis criterion #eman#s that the #eri1ati1e of theenergy function is negati1e!
Assuming a zero #am&ing factor D
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G'I9 SA3II* /+-A+,/M/+3* A/'+AI+G I+/'IA
A! '() in Parallel *ith +ther achines
With fi6e# 72 VSG was not ableto reco1er from the fault as
shown in 5ig! "!
the alternating inertiascheme im&ro1e# the stability ofthe a#$acent machine by the e6tra #am&ing effect im&ose#on the transient energy #irectly
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3! '() as an -nterace /etween the () and )rid
System with fi6e# inertia an# a zero#am&ing factor was unable toreco1er from much mil#er faults
oscillation was su&&resse# by thealternating inertia scheme2 an# these1ere transient of #c
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/=P/'IM/+A '/SUS
with fi6e# moment of inertia of;!>?@ %gm" an# D & "0 pu.
When the &ower referenceincrease#2the VSG out&ut &ower followe#the &ower comman# after&assing se1ere oscillations withthe am&litu#e of " %W
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with alternating J and D & "0 pu
he effecti1eness of the alternatinginertia in the smooth transition ofcurrent le1el an# re#ucing the 1oltageri&&les at the VSG terminal is ob1iousin this figure
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o clarify the #am&ing effect of the alternating inertia scheme
With 9: ;2 alternating inertiathe VSG can trac% the&ower reference with negligibletransients!
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,.+,USI.+
!3y selecting a big 1alue for the moment of inertia #uring acceleration2 the haste was mitigate#2 an# on the other han#2 #uring #eceleration2 a small 1alue for inertia factor was a#o&te# to increase the #eceleration effect
"!In the case of a real synchronous machine2 this transient energy is #issi&ate# by
#am&ing terms #uring .scillations
@!,om&are# to normal #am&ing factor D, the #am&ing e6erte# by alternating inertia is consi#erably more effecti1e an# has i#entical results in any con#itions!
!Any transients can be eliminate# before a&&earing! he i#ea #oes not only stabilize the VSG unit2 but also enhances the stabilit y of other machines in the system