Validating Transmission Line Impedances Using Known Event Data

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Validating Transmission Line

Impedances Using Known Event Data

Ariana Amberg, Alex Rangel, and Greg Smelich

Schweitzer Engineering Laboratories, Inc.

Copyright © SEL 2012

Why Are Line Impedances Important?

Used in distance element operation

ρ = Z

0L

= k0 = Z

APP

Can cause overreach or underreach

1

Solving for Line Impedances

Traditional Method Is Prone to Errors

Can be complex and tedious z aa z bb z cc

  r a

 r d

 j k ln

D e

D sa

  r b

 r d

 j k ln

D e

D sb

  r c

 r d

 j k ln

D e

D sc

/ mile

/ mile

/ mile z ab r d j k ln

D e

D ab

/ mile z bc r j k ln

D e

D bc

/ mile z ac r j k ln

D e

D ca

/ mile where:

2

Software Tools Improve Analysis

• Number and type of phase and ground conductors

(databases included)

Distances

• Ground resistivity

• Bundling • Line segment models

Test Equipment Measures Impedances

Test Set Test Set

V

1

2

3

V

1

2

3

Single-Phase-to-Ground Test Phase-to-Phase Test

Test Set

V

1

2

3

Three-Phase-to-Ground Test

7 tests

(no mutual coupling)

• 21 tests

(mutual coupling)

3

Ground Resistivity ( ρ) Depends on

Soil Moisture and Temperature

Courtesy of the FCC Encyclopedia

Utility Survey Results

10 to 200

Ω-m

Various methods

♦ Use single ρ value everywhere

Measure areas of system and use generalized

ρ values across those areas

Measure average across system and use everywhere

♦ Measure at new stations or along right of way

4

Measure ρ: Wenner Four-Point Method

V Ground x x x x

Probes

• Outer probes generate known current

• Voltage is measured between inner probes

• ρ is calculated from resistance as well as spacing and depth of probes

+

Each modeled with:

– Continuous ground wire

– Segmented ground wire

– No ground wire

How Important Is ρ?

• 1 ≤ ρ ≤ 100

No change in Z

1L

Big change in Z

0L

♦ Resistance 148%

♦ Reactance 144%

More effect on lines with segmented or no ground wires

5

Validate Impedances Using Event Data

Data Needed After Line-to-Ground Fault

• Voltages and currents from both ends

• Known fault location

Bus S Bus R m

S R

E

1S

Z

1S

Solve for Z

2L

and Z

0L

N1 m • Z

1L

(1 – m) • Z

1L

E

1R

Z

1R

I

2S Z

2S

V

2S

+ m • Z

2L

N2

V

2F

(1

– m) • Z

2L

V

2R

+ Z

2R

I

2R

3R f

I

0S

Z

0S

V

0S

+ m • Z

0L

N0

V

0F

(1 – m) • Z

0L

V

0R

+ Z

0R

I

0R

6

Zero-Sequence Mutual Coupling Error

S

Relay

Location Line A m

Z

0M

Line B

Z

0S

S

I

0A

Relay

Location mZ

0L

F

0

I

0

(1

– m)Z

0L

I

0B mZ

0M

Z

0L

(1

– m)Z

0M

R

Z

0R

R

N

0

Zero-Sequence Mutual Coupling Error

Z

0S

S

I

0A

Relay

Location mZ

0L

F

0

I

0

(1 – m)Z

0L

I

0B mZ

0M

Z

0L

(1

– m)Z

0M

R

Z

0R

N

0

• Relay only sees I

0A

, not I

0B

• Voltage measurement includes mutual coupling

• Method does not account for mutual coupling – errors expected

7

Verify Method Through Simulation

• Create model with known data

♦ Transmission line impedances

♦ Fault location

Use negative- and zero-sequence voltages, currents, and fault location ( m ) to calculate

Z

2L

and Z

0L

Compare results to impedances in model

Calculating Error – Traditional Method

7.832

7.757

jX

Actual = 7.8

Ð

84

°

Calculated = 7.9

Ð

82

°

Misleading in rectangular form and degrees

0.815

1.099

35% Error

R

1

° 2

°

100% Error

Calculated

Actual

8

Calculating Error – Best Choice

• Polar form is more accurate

♦ Percent error for magnitude

♦ Degree difference for angle

Previous example shows

♦ Magnitude error = 1.28%

♦ Degree error = 2°

Simulation Results (Partial)

• Low errors in Z

2L

• Low errors in Z

0L

with no mutual coupling

• High errors in Z

0L

in most cases of mutual coupling (expected)

9

Three Outliers

Line length

• Number, areas, and percentage of lines coupled

New Fault Locations

Z

0L

error increases

• Interplay between currents may lead to good results despite mutual coupling

10

Conclusions From Simulations

Reliable  Z

2L

Reliable  Z

0L

with no mutual coupling

Not Reliable X Z

0L

with mutual coupling

Using Event Data

11

Event 1

• Accurate Z

2L

• Error in Z

0L

(due to mutual coupling)

Event 2

• Accurate Z

2L

• Accurate Z

0L

(no mutual coupling)

12

Event 3

Fast breaker clearing results in

Z

2L

and Z

0L

errors

Line Impedance Calculator

13

Phenomena That Can Affect Results

Nontransposed Lines

Transposition assumed in symmetrical component domain

• Errors can occur when line is not transposed

• Nontransposed lines have coupling between sequence networks

14

Nontransposed Lines

• Three-phase fault on nontransposed line generates negative- and zerosequence currents

Faults make transposed lines nonhomogeneous

Problems Obtaining Stable Data

Fast breakers

CT saturation

CVT transients

• Evolving faults

• Changing fault resistance

CVTs + fast breakers

15

Fast Breakers

• Stable voltage and current difficult to find

• Time alignment and high sampling rate important

Future Considerations

16

V

S

I

S

Use External Fault Data

I

R

V

R m

Z

L

• Trigger events on Zone 2 forward or

Zone 3 reverse

Do not need fault location

Immune to nonhomogeneity

Unstable Data With Low Sampling Rates

How to Align Data Points

• Use synchrophasor measurements

• Align prefault data, calculate time shift, and resample at higher resolution

17

Improve Mutual Coupling Results

• Error in Z

0L

when lines are coupled

• Incorporation of coupled-line current

Complications from

Multiple coupled lines

Coupling for a fraction of line length

Terminations of coupled lines at different locations than original line

Conclusions

Incorrect Z

2L

and Z

0L

can cause misoperations

• Event reports after a line-to-ground fault help to validate impedances

• Investigate any error in Z

2L

Investigate any error in Z

0L

for lines without coupling

18

19

Questions?

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