New Method for High Impedance Faults Detection Using Total Harmonic Distortion Properties and Time Variations of Current Waveform *

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Int
IJ A
ISS
ISS
ww
N
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Key
1.
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ternational
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SN(online) 2
SN(print) 216
ww.ijape.org
IJ APE Volu
New M
Usin
T
bstract) High I
thod for HIFs
tribution netwo
HD) properties
her methods is H
ywords: High I
Introducti
hen an overhe
gh impedance
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Fs is its diffi
ults is not en
nventional ove
tection is dif
cause the mai
ermal and me
Fs due to low
network and th
tection is hum
zards as a resu
Fault impedan
sistance and r
sistance is hig
ntact with the
rbide producti
d other reaso
used the curren
rmonics in cur
e HIFs detecti
nlinear loads
me properties
enomenon sho
Several algor
l Journal o
1, Issue 7, O
161-5055
61-6442
ume 1, Issue 7
Metho
ng Tot
Time V
Department of
Impedance Fau
detection in d
orks such as cap
and time variat
HIFs detection f
Impedance Fau
on
ad conductor i
object such a
hes ground, a
icult detection
nough and ge
er current dev
fferent from L
n purpose for
echanical dam
level fault cur
heir equipmen
man lives’ pro
ult of the arcin
nce in HIFs is
resistance betw
ghly nonlinea
e earth during
ion are due to
ons [2]. Non-
nt waveform d
rrent waveform
ion. However
switching and
s as HIFs an
ould be separa
rithms and tec
f Automati
October 2012
7 October 201
od for
tal Har
Variat
Vahid Na
f Electrical & C
ults (HIFs) dete
distribution netw
acitors switchin
tions of current
from random no
ults (HIFs); Tota
in distribution
as branches of
HIF occurs.
n, because th
enerally cann
vices. The mai
Low Impedan
r LIFs detectio
mages to netw
rrents do not c
nt, but the mai
otection and
ng phenomeno
s total of the e
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distortion. Thi
ms which are
r phenomena
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ated from it.
chniques hav
on and Pow
2 PP. 165-17
12 PP. 165-17
High
rmoni
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ayebi, Majid Ga
Computer Engin
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al Harmonic Di
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Basic proper
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on is preventi
work, howeve
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in purpose for
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on [1].
earth resistanc
nd conductor
anges in cond
nsion, tubes si
enerated by th
resistance of
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good indicato
such as linea
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Fs detecting
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-- 165 --
Impe
ic Dist
of Cur
andomkar, Moh
neering, Saveh B
[email protected]

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oposed method
onlinear loads s
four stages for H
switching.
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); Time Variatio
proposed fo
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order harmo
trum [7-10],
nique [16], k
sform [18-21]
neural netwo
rithm[33-34].
n this paper the
D Properties a
stages is con
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7 October 201
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Modeling
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7 October 201
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International Journal of Automation and Power Engineering IJAPE
IJ APE Volume 1, Issue 7 October 2012 PP. 165-173 www.ijape.org ©Science and Engineering Publishing Company
- 171 -
Table 1. Circuit Line Parameters
Positive sequence resistance R
1
, Ω/km 0.01273
Zero sequence resistance R
0
, Ω/km 0.3864
Positive sequence inductance L
1
, mH/km 0.9337
Zero sequence inductance L
0
, mH/km 4.1264
Positive sequence capacitance C
1
, μF/km 0.0120
Zero sequence capacitance C
0
, μF /km 0.0075
Table 2. Loads Characteristics
Load number S ( MVA ) Cos ( phi )
1 1.75 0.85
2 1.4 0.85
3 2 0.9
4 0.87 0.86
5 0.375 0.8
5. Results
100 cases of HIF, 80 cases of nonlinear load switching, 80
cases of linear load switching, and 80 cases of capacitor
switching on the distribution network are tested. Algorithm
has been tested for M = 6 on the mentioned phenomena, which
HIFs are well separated from other same phenomena and are
detected. Some of the results are shown in the Table. 3. These
are shown that increase of current THD is permanent and
always current THD is greater than considered threshold for
nonlinear loads switching and HIFs, but that is not for linear
loads switching and capacitors switching. α and β are used for
distinction between HIFs and nonlinear loads switching. α
value is greater than 50% for HIFs and is smaller than 50% for
nonlinear loads switching. β value is greater than zero for HIFs,
but its value is zero or variable( positive and negative) for
nonlinear loads switching.
6. Conclusion
The proposed method provides a new method for HIFs
detection using FFT. The current harmonics are extracted by
using FFT and calculated current THD. Then HIFs are
detected by using four canonicals of current waveform: 1.
THD extraction, 2. Stability of THD, 3. Third harmonic of
THD, 4. Time variations. The proposed method has been
tested under many variations of networks operating conditions
including capacitors switching, linear and nonlinear loads
switching which are similar to HIFs. The results obtained from
the proposed method showed that HIFs can be detected and
easily discriminated from other same phenomena.
Table 3.Results of Proposed Algorithm for N = 1, M = 6, Threshold = 0.05
Phenomenon i = 1 i = 2 i = 3 i = 4 i = 5 i = 6
Linear load switching ΔTHD (%) 2.4 0.02 0.01 0.01 0.01 0
Capacitor switching ΔTHD(%) 3.44 0.24 0.09 0.06 0.04 0.02

Constant nonlinear load Switching
ΔTHD(%)
α(%)
I
rms
(Relaying point) (A)
3.52
16.47
351.2
3.38
14.49
351.2
3.37
14.83
351.2
3.37
15.13
351.2
3.37
15.12
351.2
3.37
15.13
351.2

Random nonlinear load Switching
ΔTHD(%)
α(%)
I
rms
(Relaying point) (A)
3.26
11.35
339.46
3.32
10.8
351.35
3.19
11.69
343.81
3.46
12.35
363.37
3.24
11.26
348.51
3.01
11.14
331.14

HIF 1
ΔTHD(%)
α(%)
I
rms
(Relaying point) (A)
3.38
97.34
344.37
3.76
97.34
348.19
3.94
97.46
355.97
4.44
97.75
359.5
4.65
97.6
361.4
4.51
97.43
359.9

HIF 2
ΔTHD(%)
α(%)
I
rms
(Relaying point) (A)
4.16
89.4
361.3
4.31
90.63
368.8
4.56
90.71
374.53
4.96
92.2
382.16
4.85
91.9
381.85
4.81
92.25
379.66

HIF 3
ΔTHD (%)
α(%)
I
rms
(Relaying point) (A)
6.14
94.6
370.21
6.69
94.81
381.62
6.87
94.78
393.57
7.08
95.15
408.46
7.12
94.35
410.47
7.45
96.68
414.53
International Journal of Automation and Power Engineering IJAPE
IJ APE Volume 1, Issue 7 October 2012 PP. 165-173 www.ijape.org ©Science and Engineering Publishing Company
-- 172 --
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Author Introduction
Vahid Nayebi was born in Iran, on Aug 02, 1987.
He received the B.Sc. degree in electrical power
engineering from the Azad University of
Technology, Saveh, Iran, in 2009. He has been
pursuing M.Sc. degree in electrical power
engineering at Azad University of Technology,
Saveh, Iran. His research interests are Microgrid and power system
protection, power system analysis.E-mail: [email protected].
Majid Gandomkar was born in Saveh, Iran in
1973. He received his B.Sc and M.Sc. degrees in
electrical power engineering from Sharif University
of Technology 1995 and 1997 respectively and PhD
degree in electrical power engineering from
Science and Research Campus, Tehran, Iran.
Currently he is an Assistant Professor with Saveh Azad University of
Technology. His research interests are distribution system, Microgrid
and power system protection.
Mohammad Javad Ramezani was born in Iran,
on July 13, 1985. He received the B.Sc. degree in
electrical power engineering from the Azad
University of Technology, Saveh, Iran, in 2008. He
has been pursuing M.Sc. degree in electrical power
engineering at Azad University of Technology,
Saveh, Iran. He was a power engineer in powerhouse, Tehran, Iran,
from 2008 to 2010. Also, He is a manager of Electrical and
Instrument Group in Iranian Offshore Engineering & Construction
Company (I.O.E.C), from 2010. His main research areas are power
systems fault diagnosis, Microgrid and power system protection and
automatic event analysis.

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