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Zed-Meter: Basic Operation

Eskom Workshop

July 2014

(2)

Overview of presentation

What is the Zed-Meter

Basic Principle of Operation

Typical Waveform

Zed-Meter Instrument &

Accessories

Lead Orientation

Software

Calibration Test

(3)

3

© 2014 Electric Power Research Institute, Inc. All rights reserved.

What is the Zed-Meter®

The Zed-Meter® is an instrument that

measures the grounding impedance of

transmission line towers

Differs from conventional methods by:

• Not requiring the removal or isolation of shield

wires

• Providing the impedance value of grounding -

most relevant for lightning performance, not

power frequency resistance

(4)

Ground Resistance vs. Ground Impedance

Conventional instruments for measuring earth

resistance operate at low frequencies (typically

105 to 150 Hz)

These instruments only provide the potential rise

of the IR term:

(5)

5

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Philosophy Behind Zed-Meter

The lightning performance (number of flashovers) of

transmission lines is related to the values of the tower

grounding impedance along the line length

High-frequency response of the ground electrode is

important

Difference between the lightning impedance of a

transmission tower grounding system and the impedance of

the same system at power frequency.

(6)

Philosophy Behind Zed-Meter (cont.)

Under lightning the peak stress on insulators occurs before

adjacent towers have had a chance to react and help out

by sharing the surge current.

2µs -two-way propagation time to the nearest pair of

towers, 300 m or 1000’ away

Under low frequency the impedance of the grounding

system at a particular structure is determined by the

parallel combination of the impedance of the local ground

electrode and the chain impedance of many towers

connected in parallel via the overhead ground wires.

Parallel chain impedance of neighboring structures is

usually much lower than that of the local ground

(7)

7

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Important Features

Does not require shield (static) wires to be removed

Provides an indication of lightning performance

Faster to implement – i.e. Lower Cost

Non-Lethal Voltages for operator and public safety

Small / Flexible Lead Foot Print

limited to ROW

Portable – does not require large power supply

(8)
(9)

9

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Basic Principle of Operation

• Inject a “lightning-like” transient current into the

tower base

• Measure the potential rise at the tower base

relative to remote ground

• Compute the ratio of the potential rise to input

current as a function of time

• Impedance measurement taken after effect of the

tower surge response has rung down.

• Impedance measurement taken before the effects

of adjacent towers have time to affect the reading

(10)

Equivalent Circuit

Propagation line

Z

Propagation line

Z

Ground wire

Z

gw

Ground wire

Z

gw

Potential Lead

Current Lead

Connection to

the structure

Voltage measurement

Propagation line

Z

Propagation line

Z

Ground wire

Z

gw

Ground wire

Z

gw

Potential Lead

Current Lead

Connection to

the structure

Voltage measurement

Current waveform

(11)

11

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Schematic Connection Representation

Current Lead

Connection

Potential Lead

to structure

Zed-Meter

90

o

-180

o

90-125 m

90-125 m

Current Lead

Connection

Potential Lead

to structure

Zed-Meter

90

o

-180

o

90-125 m

90-125 m

(12)

How the Zed-Meter Works:

Apply Pulse

(13)

13

© 2014 Electric Power Research Institute, Inc. All rights reserved.

How the Zed-Meter Works:

Pulse Moves at Speed of Light up Tower

(14)

How the Zed-Meter Works:

Other Three Legs Now Absorb Current

(15)

15

© 2014 Electric Power Research Institute, Inc. All rights reserved.

How the Zed-Meter Works: Speed along

Reaction Wire is Less than Speed of Light

(16)

Time to use

Measurement

How the Zed-Meter Works: Overhead

Groundwire Surge Impedance is Constant

(17)

17

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Time to use

Measurement

How the Zed-Meter Works:

Situation Stable for “Long” 600-ns Time

(18)

Time to use

Measurement

How the Zed-Meter Works:

Remote Potential Settles to Constant Value

(19)

19

© 2014 Electric Power Research Institute, Inc. All rights reserved.

(20)
(21)

21

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Resistor Test

Test instrument before going out into the field

Potential Lead

Connection to the structure

Current Lead

(22)
(23)

23

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Open circuit testing of leads

Measure voltage on leads

Voltage on the leads caused by electromagnetic coupling to the

energized phase conductors of the line

Potential > 50 Vrms, most utilities call for the use of insulating

gloves or other countermeasures

Zed-Meter can generate good results even if the induced pickup

exceeds 100 V because the current transducers are dielectrically

isolated from the leads

(24)

Zed-Meter Software: Standard

Testing

(25)

25

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Dipole Test

Test integrity of lead layout

Impedance of the two leads are measured.

Provides information on the condition of the current and potential leads

and the adequacy laid out pattern utilized

Current in both leads should be the same

Currents and voltage should rise quickly, stabilize within 500 ns, and

should remain relatively constant for at least 300 ns

(26)

Lead arrangements for Tests on Towers with

Buried Counterpoise

Causes coupling between test leads and counterpoise

wires

Tends to reduce the measured impedance, resulting in a

low estimate of the actual impedance

In such cases orientate test leads at right angles to the

counterpoise to reduce coupling.

(27)

27

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Lead Orientation

Current lead

Potential lead

Li

ne d

ir

ec

ti

o

n

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

Current lead

Potential lead

Li

ne d

ir

ec

ti

o

n

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

Current lead

Potential lead

Li

ne d

ir

ec

ti

o

n

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

Current lead

Potential lead

Li

ne d

ir

ec

ti

o

n

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

(28)

Lead Orientation: Zigzag Leads

Current lead

Potential lead

Li

ne d

ir

ec

ti

o

n

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

Current lead

Potential lead

Li

ne d

ir

ec

ti

o

n

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

ZZ1: In line:

Meander Potential

lead

Current lead

Potential lead

Li

ne d

ir

ec

ti

o

n

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

Current lead

Potential lead

Li

ne d

ir

ec

ti

o

n

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

ZZ2: In line:

Meander Both

leads

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Connection to

structure

ZZ3:

Perpendicular:

Meander Potential

lead

Current lead

Li

ne d

ir

ec

ti

o

n

Zed-Meter

Current lead

Li

ne d

ir

ec

ti

o

n

Zed-Meter

ZZ4:

Perpendicular:

Meander Both

(29)

29

© 2014 Electric Power Research Institute, Inc. All rights reserved.

(30)

Zed-Meter Software: Oblique

Shortened Lead Method

(31)

31

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Oblique Shortened Lead Method: Test

Features

Structure Impedance

Soil Resistivity

(32)

Differences between Standard and Oblique lead

Layouts

(33)

33

© 2014 Electric Power Research Institute, Inc. All rights reserved.

(34)
(35)

35

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Field Guide: Oblique Shortened

Lead Method

(36)

Zed-Meter Software: Oblique

Shortened Lead Method

(37)

37

© 2014 Electric Power Research Institute, Inc. All rights reserved.

(38)

Tower to Counterpoise Measurement:

Lead Connection

(39)

39

© 2014 Electric Power Research Institute, Inc. All rights reserved.

(40)

Grounding of Current and Potential Leads

In most cases it is not necessary to ground

(unless you are

using the Oblique method)

Impedance measurement is usually performed in the

time before the reflection from the end of the lead returns

back to the measuring point

Both wires are essentially “grounded” through their

capacitance to ground

(41)

41

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Connection to Structure

(42)

Conducting objects in Proximity to the

Zed-Meter® Leads

Presence of conducting objects, such as fences, vehicles

will tend to reduce the measured potential rise

Coupling

Recommended that the lead be separated from any large

conducting objects by at least 1 m.

(43)

43

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Zigzag Leads – Effect of Zigzag (Results [

Ω])

Soil Resistivity

50

Ωm

1000

Ωm

20,000

Ωm

Reference

Configuration

5 Ω

46 Ω

261 Ω

ZZ1

5 Ω

47 Ω

262 Ω

ZZ2

4 Ω

48 Ω

252 Ω

ZZ3

5 Ω

47 Ω

261 Ω

ZZ4

5 Ω

46 Ω

248 Ω

(44)

Lead Length: Shorter Potential Leads

Studied Configurations:

PL75 – Potential lead: 75 m

PL50 – Potential lead: 50 m

PL25 – Potential lead: 25 m

(45)

45

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Effect of shorter Potential Leads –Results [

Ω]

Config.

Ground

Reference

Configuration

PL75 –

Potential lead

75m

PL50 –

Potential lead

50m

PL25 –

Potential lead

25m

50

Ωm

5

5

5

5

1000

Ωm

46

46

45 (-2.2%)

43 (-6.5%)

20000

Ωm

261

257 (-1.5%)

238 (-8.8%)

202 (-22.6%)

(46)

Typical Waveform

Initial transient

from structure

Reflection from end

of current lead

Measurement

window

Actual

Measurement

interval

5

10

15

20

25

30

V

ol

tage [

V

],

I

m

pedanc

e[

ohm

]

400

600

800

1000

1200

1400

1600

1800

C

u

rre

n

t [

mA]

Tower Voltage

Tower Impedance

Structure Current

Lead current

(47)

47

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Comparison of Zed-Meter® Impedance with

Independent Measurement at Low Frequency

0,1

1

10

100

1000

0,1

1

10

100

1000

Footing Impedance,

Ω (Zed Meter Result)

F

o

o

ti

n

g

R

esi

st

an

ce,

(O

bl

ique

/

Fa

ll

of

P

ot

e

nt

ia

l M

e

thod)

Field Trial 1

Field Trial 2

Field Trial 3

Field Trial 4

Compact Electrodes (Towers)

Zed < R

(48)

Comparison of Zed-Meter® Results with Low-Frequency

Resistance Measurements for Distributed Electrodes with

Long Buried Wires

10

100

F

o

o

ti

n

g

R

esi

st

an

ce,

(R

ef

er

en

ce M

et

h

o

d

)

Radial Wires <40m

Radial Wires >40 m

Continuous Counterpoise

Distributed Electrodes

Zed > R

(49)

49

© 2014 Electric Power Research Institute, Inc. All rights reserved.

Low Frequency/High Frequency Summary

Zed-Meter works in the correct frequency / time range for

lightning.

Results for concentrated electrodes (20’ tower legs) track

low-frequency results

Results for distributed electrodes (counterpoise) will be

quite different.

Some grounding improvements that are effective for 60 Hz

(counterpoise near stations) are less effective for improving

lightning performance

(50)

Reference Material

Zed-Meter Application Guide (#1020243)

(51)

51

© 2014 Electric Power Research Institute, Inc. All rights reserved.

References

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