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Page 1: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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New Setting Free Algorithm for Out of Step Tripping

Sept. 2009 MOSCOW

H Kang – ART Areva T&D

B Cvorovic, P Horton- SAS Areva T&D

Page 2: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Introduction

Recoverable and non-recoverable power oscillations

Page 3: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Power Oscillations - Causes

What causes power oscillations?

Imbalance in generation and load

Faults (internal and external)

Load/Line switching

Page 4: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Power Oscillations – Definition (1)

Nature and definition of power oscillations

Power oscillation that leads to system split is called:

Out of step condition or pole slip or non-recoverable swing

Power oscillation that will not cause system split are called:

Stable swings or Recoverable swings

Page 5: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Power Oscillations – Definition (3)

Out of step condition

Occurs when two internal voltages of equivalent sources are in opposite direction

At that point the phase (swing) current is maximum

The position of the electrical centre will depend on Zs/Zr ratio

Recoverable swings

Two voltages typically oscillate between up to 120deg

VrVsZs Zr

OST condition :

I=(Vs -Vr )/ZT =(Vs -(-Vr ))/ZT ~2 Vn /ZT

ZT =Zs +Zline +Zr

Electrical. center

Page 6: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Elliptic shape: recoverable swing

Circle: OST condition

Power Oscillations – Definition (4)

Page 7: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Power Oscillations – Definition (5)

Recoverable

Non-Recoverable

Page 8: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Traditional Out of Step Detection Methods

Page 9: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Conventional methods:

Conventional methods use blinders to determine speed of impedance crossing the ∆R region (R6-R5). They may predict or detect OST condition.

If polarity of ‘R’ has changed on exiting Z5, it is Out of Step condition (already happened)

If positive sequence impedance crosses ∆Z region faster than ‘delta T’ set time the predictive OST is declared

Disadvantages

Difficulties to set blinders due to heavy loading

Setting dependant on system topology, thus settings may be inaccurate

Comprehensive system study required – increases the engineering time

Prone to unstable operation in series compensated lines during MOV operation

Out of step tripR

Z5

ZL

Z6

Z5'

Z6'

R5 R6R5'R6'

Predictive Out of step trip

+jX

Recoverable swing

Disadvantages

Page 10: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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New algorithm provides:

Setting free OST detection

CB tripping at a favourable angle

New Algorithm

Page 11: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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New Algorithm - Principle

Setting Free OST Detection Principle

Page 12: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Setting Free OST Detection – Principle (1)

OST detection principle:

Recoverable swings: ∆R changes polarity when ∆I changes polarity

Non- recoverable swings: ∆R doesn’t change polarity when ∆I changes polarity

I=positive sequence currentR=positive sequence resistance

RECOVERABLE SWING:Point when both, ∆I and∆R change polarity

Point when ∆I changes polarity and ∆R polarity

remains unchanged

NON RECOVERABLE SWING:

R

jX ∆I=IN+1-IN∆R=RN+1-RN

Page 13: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Recoverable Swings

Delta I and Delta R change polarity around same time

Pole Slips

When Delta I changes polarity , Delta R does not

Recoverable Swing Pole Slip

Setting Free OST Detection – Principle (2)

Page 14: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Tripping Angle Control

Circuit breaker tripping angle control

Page 15: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Tripping Angle Control

Vs Vr

Current Locus (I)

90

180 (minimum Z)

Vr locus Electrical Centre locus

0

180

90

180

90

X

270

270

270

Current locus during oscillation is a circle

Drawing taken from Westinghouse book

Page 16: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Tripping Angle Control (1)

Current during oscillation can be defined as:

I swing=IMAX sin (θ/2)

where θ is the angle between internal voltages of sources

Imax

I240

90

240

180

270

0

Page 17: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Tripping Angle Control (2)

I trip=IMAX sin (240/2)=0.866 IMAX

Maximum phase (swing) current is recorded at the point when ∆I changes polarity (that point corresponds to minimum impedance)

Favourable (safe) split angle entered, for example 240 degrees

Tripping command is issued when phase current drops to:

Page 18: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Supporting Elements(1)

Power Swing Detection and Blocking

Page 19: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Supporting Elements(2)

Page 20: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Supporting Elements(3)

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Proof of Concept

Pole slip COMTRADES captured by the relays for various system tests were used to prove that the basic principle was sound

Modifications were made to the original principle to make it more robust.

Logic implemented to account for difference between the frequency of I and V during swings

Logic to make the algorithms immune to system disturbances and faults

Page 22: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Test Results (1)

Numerous cases from different systems were applied

Algorithm remains stable during power system faults or recoverable swings

Both, balanced and open pole oscillation tested

No mal-operation recorded during evolving faults, sudden change of power flow, cross country faults and frequency variations

Angle set tripping compared with actual angle across the breaker proved to be accurate

Page 23: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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S w i n g / P o l e S l i p I

O S T

Test Results (3)

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Test Results (4)

Page 25: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Test Results (2)

Page 26: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Conclusions

Page 27: 11 New Setting Free Algorithm for Out of Step Tripping Sept. 2009 MOSCOW H Kang – ART Areva T&D B Cvorovic, P Horton- SAS Areva T&D

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Setting free

All conventional methods require system studies and comprehensive settings

No blinders, no starters, thus no constraints on operating characteristics versus loading

Immune to topology changes

Security – Provides control over the angle at which the system is to be split.

Minimises chances of breaker opening at voltage maximum

Advantages

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Thank You

Questions?