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电力系统震荡与失步(POWER SWING AND OUT-OF-STEP CONSIDERATIONS )

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发表于 2007-12-31 22:24:33 | 显示全部楼层 |阅读模式
论文文献
标题: 电力系统震荡与失步(POWER SWING AND OUT-OF-STEP CONSIDERATIONS )
作者: IEEE
所属专业方向: 电力系统
摘要: 介绍电力系统震荡与失步诊断与措施(POWER SWING AND OUT-OF-STEP CONSIDERATIONS )
关键字: 电力系统 震荡 失步
来源: IEEE

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IEEE 有关电力系统震荡与失步方面的好文章(POW Power System Swing & OOS.rar (623.47 KB, 下载次数: 13) ER SWING AND OUT-OF-STEP CONSIDERATIONS )
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 楼主| 发表于 2008-1-19 12:33:35 | 显示全部楼层

论文摘要

4.2 ADDITIONAL POWER SWING DETECTION METHODS1 w# z  g) z8 T$ [/ v8 \5 A
4.2.1 Continuous Impedance Calculation/ R: u* o/ `' F: e. r4 [4 L0 j
This method determines a power swing condition based on a continuous impedance calculation.& H. m1 h/ Q+ E) y9 N. B0 ?+ m2 c
Continuous here means, for example, that for each 5 ms step an impedance calculation is
. V$ w2 p. c; [( p( _1 P# c+ Gperformed and compared with the impedance calculation of the previous 5 ms. As soon as there is& c3 E' k4 _( i. V) A
a deviation, an out-of-step situation is assumed but not proven yet. The next impedance that" `/ \2 F3 k6 P- ]7 I/ h# J
should be calculated 5 ms later is predicted based on the impedance difference of the previous
2 X- J7 g' w$ \* W4 F6 Y# P, mmeasured impedances. If the prediction is correct, then it is proven that this is traveling impedance.
7 R+ r+ X. }3 b/ K4 vIn this situation a power swing condition is detected. For security reasons additional predictive
/ y- H  ^( M9 h; U# m* Ccalculations may be required.+ ]& M6 M3 D2 A4 ]/ J+ @+ z
A delta impedance setting is not required anymore, because the algorithm automatically considers% w# o9 ~0 S5 y, i9 p+ e
any delta impedance that is measured between two consecutive calculations and sets the delta% c; Q# M% q8 T  N2 g
impedance for the next calculation automatically in relation to the previous calculation. This leads+ z. u0 `  @, m; P- X5 B
to a dynamic calculation of the delta impedance and an automatic adaptation to the change of the. F1 P& d8 A) b+ M; P5 \
power swing impedance. Also the delta time setting is not required anymore because it is
; X& s7 b  \, O: w* J4 J$ H1 zdetermined by the calculation cycles of the algorithm.
% F3 R1 ~$ C- l# q4 w! ?R
! ?. G- V- L7 `+ D* _2 NX! U; P  Q' }  e1 ?! P( {& u
Stable power swing
/ c1 f) r/ @2 K& Y9 V& w! Limpedance trajectory
5 W* j: ~, O, c& n; X/ ODZ1 DZ2 DZ3
  a- u! x% z7 l: OLoad" A  W* t" E( A' F0 k
Figure 7 Power swing detection with continuous impedance calculation
. s, [5 v: u1 [9 ]1 `As long as the changing impedance vector is not approaching a tripping zone faster than the relay
. `! S1 {% |9 J; |5 r  Ocan confirm the out-of-step condition (at least 3 calculations 10 ms) the detection will be successful.3 R& N  _8 ]; E. V( A$ y- J
POWER SWING AND OUT-OF-STEP CONSIDERATIONS ON TRANSMISSION LINES# H+ j* h' T% R9 e$ L
IEEE PSRC WG D69 d' R( N0 q2 x: ?! S0 p
17 / 59 2005-07-19" n4 K) K# n# o% x) r- L; s
4.2.2 Swing-Center Voltage and its Rate of Change
  L$ U% [  c# p. B# n( q* b6 Y$ i8 vSwing-center voltage (SCV) is defined as the voltage at the location of a two-source equivalent6 ~3 d8 g* K% G, U* \1 E/ A- [9 i
system where the voltage value is zero when the angles between the two sources are 180 degrees0 E7 ~6 S, R8 \( Z& N0 `
apart. When a two-source system loses stability and goes into an OOS situation after some% W0 B5 m% m: V$ X7 U$ G6 p
disturbance, the angle difference of the two sources, d(t), will increase as a function of time. Figure
4 R2 f" h! s- U7 U8 illustrates the voltage phasor diagram of a general two-source system, with the SCV shown as) U; |+ N! P  P
the phasor from origin o to the point o'.4 A5 I8 G- y  |# @( G
o'. y+ Z- v0 [  C0 h" L  R4 K
o" `8 _: m& B% e3 x
o", x% p# `2 ?6 ]' U' a0 A1 ~
Z1S•I Z1L•I
1 G. k5 X( T" K2 d  y' `! bVS
" e6 W7 V9 d* V) V6 O9 p- K7 Rj ER+ A+ ^* O. s1 ^5 ?
d
( ?6 _& j% q3 J. d1 e2 s) DSCV
: P" z: v% F2 h. i8 K3 ~, MZ1R•I2 N6 Q: g. m8 c: A! k! {' L, C
q# d3 K: W" A& i: |; ~  a
I: M. |# a' ?" b& M
ES8 Q  i, l* h9 a3 L5 `
VR* N, V: |& E9 D. c. T7 X
Figure 8 Voltage Phasor Diagram of a Two-Source System
2 U7 {' v  W* B7 @* E% d* H9 y* uAn approximation of the SCV can be obtained through the use of locally available quantities as0 S6 w, f  b* K( x9 S
follows:
. ^& O5 v: p& P! `7 e6 kSCV »| V | ×cosj S (6)/ r( U1 h: e! m. Y2 \2 I- I" |
Where |VS| is the magnitude of locally measured voltage, and j is the angle difference between VS
6 m& b6 u- K$ x  E% x5 `8 [& Cand the local current as shown in Figure 9. In Figure 9, we can see that Vcosj is a projection of VS; g6 X+ a1 |' S/ S  ?# U; L
onto the axis of the current, I. For a homogeneous system with the system impedance angle, q,: h- K: t. c  ^7 y% c1 B
close to 90 degrees, Vcosj approximates well the magnitude of the swing-center voltage. For the
8 l( ~; W3 \8 }" G( gpurpose of power-swing detection, it is the rate of change of the SCV that provides the main
" X/ x. k- Q( y& j6 A1 q- xinformation of system swings. Therefore, some differences in magnitude between the system SCV
1 x& M8 o, C" n' d7 y" _$ B( c5 Fand its local estimate have little impact in detecting power swings. Ilar [6] first introduced the% [7 V6 J. @$ V+ h, [/ D
quantity of Vcosj for power swing detection.
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