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Technical article

March 2017

91

www.read-eurowire.com

AC cable (XLPE, 20 kV)

The test configuration consisted of two MV

cables connected together in series and of

slightly different lengths (

Figure 5

).

Parameters:

• Cable 1:

758m

• Cable 2:

708m

• Further parameters:

unknown

• AC voltage:

up to 10kV, 50Hz, connected to near

end of cable 1 (see

Figure 1

,

Figure 6

)

• Measurement equipment:

transient recorder for fault location,

broadband

divider

(resistive-

capacitive), AC high voltage divider

(undamped capacitive)

The artificial breakdown was generated

by using a spark gap (

Figure 5

) which

was installed either at the far end of

the complete cable length or at the

connection point between the two cables.

The voltage was increased up to 10kV

rms

and until the spark gap got fired. The

resulting signals of the travelling waves

were recorded.

The signals were taken from the HV circuit

using a resistive-capacitive broadband

divider (for reference measurements) or

an undamped capacitive HV AC divider of

type WCF

[6]

(

Figure 6

).

The HV divider output was connected

with the transient recorder by a coaxial

measuring cable.

The reference measurement with the

broadband divider is shown in

Figure 7

.

Thereby channel 1 (Ch1, blue) shows

the signal reflections when the spark

gap is connected at the far end of both

cables and channel 2 (Ch2, red) shows

the signal reflections when the spark gap

is connected to the connection point

between the cables.

The upper diagram is the complete signal

recording over about 300µs. In the middle

diagram the first and the second reflection

are zoomed out. In the lower diagram the

differentiated curves are shown with Ch11

related to Ch1 and Ch12 related to Ch2.

From this measurement the propagation

velocity is determined to

v

= 172.5m/µs

based on T = 17.0µs of Ch1 and according

to

Equation 2

. Now the

T

x

= 8.79µs of Ch2

indicates exactly the length of the cable

sample of 758m.

Assuming an uncertainty of ±0.2µs of the

time evaluation for both full length and

partial length, the following cable lengths

to failure can be estimated. Based on the

determined cable length of 758m the

maximum deviation is 11m, which is 0.75

per cent of the full cable length.

Furthermore, the measured signal shows

a significant decline. This comes from the

damping of the cable itself and from its

dispersion. Comparison of the waveforms

in Ch1 and Ch2 show that the reflection

losses are also a substantial part of the

cable losses, because the decrease of the

voltage as a function of the number of

reflections is more or less constant.

After

this

initial

test

the

same

measurements

with

an

undamped

capacitive divider were carried out.

The goal was to find out if it is possible

to get usable results of fault location

even with a voltage divider with a lower

bandwidth (

Figure 6

).

Figure 8

shows the results of a

measurement with a divider type WCF

normally used in resonant test systems

for cable tests. It is clear to see that such

a divider is actually not suitable for such

fast transient measurements. Nevertheless,

there is still a possibility to evaluate a fault

position. In the lower diagram of

Figure 8

the curves are filtered with a numerical

low-pass Bessel filter to find the transition

points of the reflection.

Assuming a well-known propagation speed

(172.5m/µs) the fault can be located at

759m. But it is clear that the uncertainty of

determination is much higher than before.

A second test with the same divider was

performed, but this time the divider type

WCF was damped with a resistor of 150Ω.

It is shown that the damping resistor

eliminates the majority of the oscillations

after the transition in the waveform.

Therefore, a further filtering is not

necessary for the evaluation.

Figure 5

:

AC cable with spark gap (detail)

Figure 6

:

AC source and HV divider

Figure 7

:

Measurement with broadband divider

Figure 8

:

Measurement with divider type WCF,

undamped

T

partial length

[µs]

8.77

8.79

8.81

T

full length

[µs]

v [m/µs]

calculated length [m]

16.8

170.5

748

749

751

17

172.5

756

758

760

17.2

174.5

765

767

769

Table 2

:

Calculated cable lengths for different signal propagation times

Figure 9

:

Measurement with divider type WCF,

damped with 150Ω