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This document provides an overview of key concepts related to conduction and breakdown in gases. It discusses gases as insulating media and the phenomena that occur when a voltage is applied, such as conduction and eventual breakdown if the applied voltage increases sharply. It also includes worked examples, tables providing information on liquid dielectric properties, figures illustrating breakdown channels in perspex, and multiple choice questions to help gain an overview of important chapter topics.

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Pankaj Rupani
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0% found this document useful (0 votes)
73 views4 pages

Visual Preview

This document provides an overview of key concepts related to conduction and breakdown in gases. It discusses gases as insulating media and the phenomena that occur when a voltage is applied, such as conduction and eventual breakdown if the applied voltage increases sharply. It also includes worked examples, tables providing information on liquid dielectric properties, figures illustrating breakdown channels in perspex, and multiple choice questions to help gain an overview of important chapter topics.

Uploaded by

Pankaj Rupani
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
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Contents xv

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I

2
26 High-Voltage Engineering
N
T
R
O Conduction and
D Breakdown in Gases
U
C 2.1 GASES AS INSULATING MEDIA
T The simplest and the most commonly found dielectrics are gases. Most of the
electrical apparatus use air as the insulating medium, and in a few cases other
I gases such as nitrogen (N2), carbon dioxide (CO2), freon (CCl2F2) and sulphur
6) are also used.

O Various phenomena occur in gaseous dielectrics when a voltage is applied.

N and the insulation retains its electrical properties. On the other hand, if the ap-

sharply, and an electrical breakdown occurs. A strongly conducting spark formed


during breakdown practically produces a short-circuit between the electrodes.

Chapter Introduction provides a quick look


into the concepts that will be discussed in
the chapter.

W
WORKED EXAMPLES O
Example 4.1 A solid specimen of dielectric has a dielectric constant of 4.2,
R
and tan = 0.001 at a frequency of 50 Hz. If it is subjected to an alternating K
dielectric loss.
E
Solution Dielectric heat loss at any electric stress E [Eq. (4.5)]
D
E 2 f r tan
= W/cm3
1.8 1012 E
For the specimen under study, the heat loss will be X
50 50 10 6 50 4.2 .001
=
1.8 1012
A
= 0.291 mW/cm3 M
Example 4.2 A solid dielectric specimen of dielectric constant of 4.0
P
L
E
the voltage at which an internal discharge can occur. S
Every chapter contains several worked
out Examples which guide the student in
understanding the concepts and working
out the exercise problems.
xvi Contents
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T
Table 3.1 Dielectric properties of some liquid dielectrics
A Property Transformer Cable Capacitor PETEP Silicone

B Breakdown strength
oil

15
oil

30
oil

20
oil

> 15
oils

30–40
L at 20°C on 2.5 mm
standard sphere gap
kV/mm kV/mm kV/mm kV/mm kV/mm

E Relative 2.2–2.3 2.3–2.6 2.1 2.7 2–73

10–3 0.1 10–3 10–3


S Tan
10–3 0.5 10–3 10–4
Resistivity (ohm-cm) 1012–1013 1012–1013 1013–1014 > 1014 3 1014

at 20°C

20°C (CS)
Acid value (mg/gm Nil Nil Nil < 0.03 Nil

1.6000

Thermal expansion 7 10–4/°C 7 10–4/°C 7 10–4/°C 0.00075 5


(20–100°C) 10–4/°C
Max. permissible 50 50 50 200 < 30
water content (in ppm) (negligible)

Wherever necessary, Tables provide


accurate and extensive information on the
topic discussed.

F
I
G
U
R
E
S

Fig. 4.2 Breakdown channels in perspex between point-plane electrodes.


Radius of point 0.01 in, thickness 0.19 in. Total number of impulses
190. Number of channels produced 16; (n) point indicates end of nth
channel. Radii of circles increases in units of 10–2 in.
Source: R. Cooper, International Journal of Elec. Engg. Education,
vol. 1, 241 (1963)

Well-labelled illustrations give a clear


understanding of the concepts.
Contents xvii
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M
C MULTIPLE CHOICE QUESTIONS
1. A small high-voltage laboratory usually will have
Q (a) ac, dc test sources with ratings less than 100 kV, 10 kVA./kW and
impulse of voltage 400 kV, 5 kJ
s (b) ac, dc test sources of 500 kV, 100 kVA/kW, and impulse of 1 MV,
10 kJ
(c) ac voltage sources of 300 kV, 10 kVA, and impulse voltage of
W 1 MV, 15 kJ
(d) ac, dc sources only.
I 2. Test sources required for testing power apparatus of 220 kV, 3-phase ac
system are
T (a) 500 kV ac, 1 MV impulse
(c) 300 kV ac, 500 kV impulse
(b) 800 kV impulse
(d) 250 kVA, 500 kV impulse.
H 3. The kVA rating of a testing transformer unit intended for test voltage and
test object capacitance ‘C’ (pF)
(a) C V2 (b) C V2 10–9
(c) C2 V2 109 (d) C V2 10–6.
A 4. The rating of an impulse voltage generator with generator capacitance
Cg and voltage rating V with n stages is (kJ)
N (a) 0.5 Cg V2 (b) (n/2) (Cg V2)
Cg V 2
S. (c) (d)
(Cg V 2 )
2n 2n 2

Multiple choice questions help the student


gain a quick overview of the important
topics in the chapter. Answers are also
provided at the end.

Q
REVIEW QUESTIONS U
6.1
high dc voltages.
E
6.2
proper voltage division between the valves ensured, if a number of tubes
S
T
6.3 Why is a Cockcroft–Walton circuit preferred for voltage multiplier
agram. I
6.4 Give the expression for ripple and regulation in voltage multiplier circuits.
O
N
PROBLEMS
S
6.21 An impulse generator has 12 capacitors of 0.12 F, and 200 kV
rating. The wave front and wave tail resistances are 1.25 k and 4 k
respectively. If the load capacitance including that of the test object is

impulse wave produced.


6.22 An 8-stage impulse generator has 1.2 F capacitors rated for 167 kV. What
is its maximum discharge energy? If it has to produce a 1/50 s waveform

wave tail resistances.

Review questions and problems help


students hone their problem-solving skills.
xviii Contents
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R
E REFERENCES
F 1. Alston, L.L., High Voltage Technology
E (1967).
2. Electromagnetic Fields, McGraw-Hill, New York (1960).
R 3. Kuffel E., Zaengl, W.S. and Kuffel, J., High Voltage Engineering
Fundamentals
E 4. Popovic, B.D., Introductory Engineering Electromagnetics, Addison-
Wesley (1971).
N 5. Finite Elements in Electrical and
C Magnetic Field Problems, Wiley-Interscience Publication, John Wiley and
Sons, New York (1980).
E 6. Silvester, P.P. and Ferrari, R.L., Finite Elements for Electrical Engineers,

S 7. Binns, K.J. and Lawrenson, P.J., Analysis and Computation of Electric


and Magnetic Field Problems
8. The Finite Element Method in Engineering Science,
McGraw-Hill, London (1977).

IEEE Transaction on power apparatus and systems, 97, 1156–


1166 (1977).

Extensive list of References helps in


selecting books for further study.

A
P
Appendix Appendix 463
P
E
N
Important Formulae D
I
X
Field Enhancement Factor
Emax
f=
Eavg.

Townsend current growth equation


I = I0 exp ( d)
Current growth in presence of Secondary Processes
I 0 exp ( d )
I=
1 exp ( d ) 1

Appendix at the end lists important


Formulae and Symbols.

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