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International Journal of Applied Power Engineering (IJAPE)
Vol. 3, No. 2, August 2014, pp. 115~123
ISSN: 2252-8792  115
Journal homepage: http://iaesjournal.com/online/index.php/IJAPE
Assessment of Electric Field Distribution Inside 500/220 kV
Open Distribution Substations during Working Conditions
Sayed A. Ward , Samy M. Ghania, Essam M. Shaalan
Electrical Engineering Department, Faculty of Engineering at Shoubra Benha University, Cairo, Egypt
Article Info ABSTRACT
Article history:
Received Mar 2, 2014
Revised Jul 10, 2014
Accepted Jul 23, 2014
The high level electric field intensity produced by high voltage (HV)
equipments inside 500/220 kV substations is harmful for the human (staff)
health. Therefore the minimum health and safety requirements regarding the
exposure of workers to the risk arising from electric fields produced inside
these substations is still considered as a competitive topic for utility
designers, world health organization (WHO) and biomedical field
researchers. It is very important to have knowledge about levels distribution
of electric field intensity within these high voltage substations as early stage
in the process of substation design. This paper presents results of
investigation 50Hz electric field intensity distribution inside 500/220 kV
power transmission substations in Cairo, Egypt. This paper presents a
method for assessment the distribution of 50HZ electric field intensity
distribution inside this substation, this method of analysis is based on the
charge simulation technique (CSM). This study will serve for planning
service works or for inspection of equipment on HV power transmission
substations.
Keyword:
Charge simulation technique
Electric field intensity
High voltage substations
Copyright © 2014 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Essam M. Shaalan,
Electrical Engineering Department, Faculty of Engineering at Shoubra,
Benha University,
Cairo, Egypt
e-mail: essam.shihata@feng.bu.edu.eg
1. INTRODUCTION
Powerful electric systems with very high voltage are the source of harmful electromagnetic field
radiation. This is because these electromagnetic field radiations represent the primary source to the resultant
electrical current induced in the human body under or near electric power systems [1]. Therefore, the
problem of the human exposure to electric fields has become more important with increasing the number and
the size of power substations and electric power systems in general. This harmful attract an increased
attention of many biomedical field researchers, scientific research communities worldwide on the health
effects of electric power systems. As a result of this interest, the governments are playing an active role in the
reduction of these exposures to electric fields by setting exposure limits for such fields which resulting from
different electrical power systems [2-4], to guarantee the life insurance of all staff working inside these
substations.
The 50 Hz electromagnetic field is distributed unevenly in space between separate power
installations inside HV substations. In open 500/220 kV power transmission substations, the sum of
electromagnetic field sources with grounded metal constructions creates a complex picture of the electric
field. Works are connected with operative switching, equipment inspection; different repair work, etc. require
presence of staff personal in various points of 500kV & 220kV Switchyards (substation territory). Therefore,
the investigation of the distribution levels of the electric fields inside these substations is an important step
for solving the problem of personnel protection from the effects of these fields.
 ISSN: 2252-8792
IJAPE Vol. 3, No. 2, August 2014 : 115 – 123
116
In this paper, the present algorithm is carried out to assessment the distribution levels of the electric
field intensity produced by different high voltage electrical power systems inside 500/220 kV air-insulated
substation (AIS). In addition to the investigation of levels distribution of electric field intensity inside
500/220 kV AIS at 1.5 m from ground surface, we will also investigate the distribution levels of electric field
intensity during different working conditions and at different positions inside this substation. These
calculated levels will be compared to the standard limit levels stated by international organizations [2-4].
This developed method is based on the charge simulation technique, which simulate the typical 500/220 kV
substation with all incoming and outgoing feeders by developing multi-scripts of m-file Matlab software
package to calculate the distribution levels of electric field intensity inside this substation. This method is
considering the complex systems, including three-dimensional multiple incoming, outgoing overhead lines
and bus system inside this substation.
2. SUBSTATION DESCRIPTION AND SYSTEM MODELING
The calculations of electric fields are performed inside 500/220 kV AIS, Cairo 500 substation. This
substation is supplied by four 500 kV overhead transmission lines, single circuit, which are connected to the
same 500 kV double bus systems, main and standby bus-bars. This substation has three identical 3-ph, 500
MVA, 500/220/11 kV power transformers installed inside it, each one is composed of three single phase
transformers. This substation is supplying six loads through six 220 kV double-circuit overhead transmission
lines which are outgoing from the same 220 kV double bus systems, main and standby bus-bars. This
substation has a simply 500 kV,220 kV bus systems with 300 m long and 12 m, 9m height respectively.
Single line diagram for this substation is presented in Fig. 1.
The location of equipment in the open distribution substation, as usual, is asymmetrical. Some
equipment is often locates in separate groups. Between these equipments, there are a complex system of
busbar, incoming and outgoing feeders which are similar to the web covering all open distribution substation.
This complicates the task of investigation the fifty hertz electric field intensity.
The human body is allocated within the highly exposure zones of electric fields inside this
substation and at different heights to determine the field distribution levels during different working
conditions, Fig. 2.
Works are connected with operative switching, equipment inspection; different repair work, etc.
require presence of staff personal in various points of 500kV & 220kV Switchyards (substation territory).
Therefore, the investigation of the distribution levels of the electric fields inside these substations is carried
out during different working conditions for staff.
The first Scenario is carried out at a height of 1.5 m above the ground level which presents worker
(staff) standing with his foot on ground inside switchyards during normal operation and (hot-stick position)
during live- working conditions (Scenario 1).
The second Scenario is carried out at a height of 11 m for 500 kV switchyard and 8.5 m for 220 kV
switchyard, which presents the position of the worker (staff) in (bare hand position) during live maintenance
conditions for 500 kV and 220 kV bus systems (Scenario 2).
The third Scenario is carried out at a height of 17 m for 500 kV switchyard and 14 m for 220 kV
switchyard, which presents the position of the worker (staff) in (bare hand position) during live maintenance
conditions for 500 kV and 220 kV incoming and outgoing feeders (Scenario 3).
In the electric field model presented in this paper, 500 kV bus-bars (HV bars) and 220 kV bus-bars
(LV bars), incoming 500 kV feeders and outgoing 220 kV feeders are approximated by internally located line
charges. Such a simplification is acceptable when the field is analyzed at a long enough distance from the
conductor, e.g. near the ground surface. The electric potential of incoming 500 kV feeders, outgoing 220 kV
feeders and bus-bar surfaces has been defined as complex potentials and assumed to be equal to their phase
voltage. These assumptions lead to a charge simulation method formulation. The standby bus-bars are
represented by line charges, their potential is assumed to be zero. The influence of tower insulators is
neglected when the field is calculated. In this paper the HV systems of alternating current are considered,
therefore the potential and charge densities are complex quantities.
In this paper the Charge Simulation Method is used to compute the electric fields [5], where the live
conductors are simulated by a number of discrete simulation charges located on the axis of these conductors.
Values of simulation charges are determined by satisfying the boundary conditions at a number of contour
points selected at the conductor surfaces.
Once the values of simulation charges are determined, then the potential and electric field of any
point in the region outside the conductors can be calculated using the superposition principle using the
following equations:
IJAPE ISSN: 2252-8792 
Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution… (Essam M. Shaalan)
117
Figure 1. Single line diagram of simulated 500/220 kV AIS substation, Cairo 500 substation.
]][[][ QPV  (1)
Where: [Q] is a column vector of the fictitious simulation charges, [V] is a column vector of the potential
given by the boundary conditions and [P] is the matrix of the Maxwell potential coefficients which depend on
the type of fictitious simulation charges [5, 6].
In our developed model, we simulate HV and LV bus-bars, incoming 500 kV feeders and outgoing 220 kV
feeders by internally located line charges on their axes. Therefore the potential coefficient is given by [7]:









))((
))((
ln
4
1
221121
221121
dLLdLL
dLLdLL
d
Pij

(2)
 ISSN: 2252-8792
IJAPE Vol. 3, No. 2, August 2014 : 115 – 123
118
Where
2
1
2
1
2
11 )()()( ZZYYXXL 
2
2
2
2
2
22 )()()( ZZYYXXL 
2
1
2
1
2
111 )()()( ZZYYXXL 
2
2
2
2
2
222 )()()( ZZYYXXL 
2
21
2
21
2
21 )()()( ZZYYXXd 
Figure 2. Different positions of the workers during different working conditions.

































































2)(1)(
4
1
2)(1)(
4
1
2)(1)(
4
1
22
2
11
1
2
2
1
1
22
2
11
1
2
2
1
1
22
2
11
1
2
2
1
1
L
ZZ
L
ZZ
L
ZZ
L
ZZ
d
F
L
YY
L
YY
L
YY
L
YY
d
F
L
XX
L
XX
L
XX
L
XX
d
F
z
y
x



(3)
Where
)(
1
)(
1
1
2121 dLLdLL 



)(
1
)(
1
2
22112211 dLLdLL 



Therefore the net field (Ei) at any point (Pi) due to a number of individual charges (n) each with charge of
(Qj.) is given as:
      z
n
j
jzijy
n
j
jyijx
n
j
jxiji aQFaQFaQFE  

111
*)(*)(*)( (4)
Where (Fij)x, (Fij)y and (Fij)z are the „field intensity‟ or field coefficients and ax, ay and az are unit vectors in
the x, y and z directions, respectively [7].
The total electric field at the ith
contour point is expressed as:
IJAPE ISSN: 2252-8792 
Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution… (Essam M. Shaalan)
119
222
( ziyixii EEEE  (5)
3. SIMULATION RESULTS AND DISCUSSIONS
This study was conducted not only for a workers standing on the ground surface with his foot in
switchyards during normal operation and (hot-stick position) during live- working conditions (Scenario 1),
but also for a workers in live line maintenance position (bare hand position), at a height of 11 m for 500 kV
switchyard and 8.5 m for 220 kV switchyard (Scenario 2) and at a height of 17 m for 500 kV switchyard and
14 m for 220 kV switchyard (Scenario 3). The human body was assumed to be standing in free space and not
in contact with electrical ground. Workers in bare-hand working operate very close to live conductors and
they wear special conductive clothing which protects them against the exposure of the electric field. These
clothes are ignored in our simulation.
The research results which are presented in this paper were carried out at the same actual schedule
of working conditions for selected substation. These results have been presented in form of the electric field
distribution maps and surface distribution (Fig. 3 & Fig. 4). The results of work are currently used for
organization of the regular works on open distribution substations. Presentation of results in the form of
maps, contours and three dimensional figures provides great visibility and a convenience in practical
application. For example, when it is necessary to select a proper route for inspection substation or when
choosing the proper protective equipment necessary for working personal without turned off above voltage,
etc.
Figure 3. Map of the electric field (V/m) distribution inside Cairo 500 substation during scenario 1.
Table 1. The Distribution of Electric Field in the Zone of Open Distribution Substation (Scenario 1).
0 50 100 150 200 250 300
0
50
100
150
200
250
300
350
400
-1000
0
1000
2000
3000
4000
5000
6000
7000
8000
9000
10000
11000
12000
13000
14000
15000
16000
17000
18000
19000
20000
21000
22000
The part of the open distribution substation
territory,%,
where the electric field is in the range (E in
kV/m)
E Range
0≤Е<5
5≤Е<10
10≤Е<15
15≤E<20
20≤E<25
25≤E<30
Territory,%, 42.3 21.5 11.3 10.7 7 7.2
 ISSN: 2252-8792
IJAPE Vol. 3, No. 2, August 2014 : 115 – 123
120
According to recommendations of SanPiN 2.2.4.1191-03 [8], employees, serving electrical installations are
permitted to:
 stay in the 50-HZ electric field with the intensity of up to 5 kV / m during the working day;
 stay in the 50-HZ electric field with the intensity from 5 to 20 kV / m during limited time,
calculated as follows:
2
50

E
T (6)
Where E is the electric field intensity in kV/m in the controlled area, T is the time in hrs.
Therefore when the electric field intensity is in range from 20 to 25 kV/m, stay of the staff in this
electric field should not exceed 10 minutes;
 Maximal permitted level of the electric field intensity in open distribution substation is 25 kV /
m.
 Staying in the electric field with the intensity of more than 25 kV / m without use of the
protective equipment is not permitted.
Going along the calculated electric field intensity, it is determined the points where the electric field
intensity reaches the maximum exposure limit values 5, 10, 15, 20 kV/m. Table 1 depicts, in percents, values
of zones with electric field intensities less 5kV/m (zone of security) and higher 5kV/m (zone of influence) at
scenario 1. Results of calculated data analysis in (Table 1) are showed that, in average; 42.3% of the open
distribution substations occupy the territory on which the electric field does not exceed 5 kV / m (zone of
security). And the territory of open distribution substations at which the electric field is greater than 5 kV / m,
where it requires limited stay time for safety performance of work, is called the zone of electric field
influence. This territory takes, in average, about 57.7% of the open distribution substation.
The distribution of the electric field intensity in the zone of electric field influence where the electric
field intensity higher 5kV/m is as follows:
 21.5% of the territory falls on the zone with the electric field from 5 to 10 kV/m,
 The zone from 10 kV to 15 kV/m is much smaller (about 11.3% of the territory of AIS).
 The zone from 15 kV to 20 kV/m is about 10.7% of the territory of AIS.
 The percentage of the zone with the intensity from 20 to 25 kV/m, where the permission stay
time is not exceed 10 minutes, is about 7% of the territory of AIS.
 The intensity of the electric field more than 25 kV/m, where the presence without personal
protective equipment is prohibited, and the value of such zones is the about 7.2% of the
territory of AIS.
Figure 4. The electric field distribution (V/m) inside selected substation switchyard during scenario 1.
Fig. 5 and Fig. 6 slow the electric field distribution inside Cairo 500 substation for the other two scenarios 2
& 3 mentioned previously, while Table 2 summarize the maximum and average electric field values for
different working conditions.
IJAPE ISSN: 2252-8792 
Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution… (Essam M. Shaalan)
121
Figure 5. Map of the electric field (V/m) distribution inside Cairo 500 substation during scenario 2.
Figure 6. Map of the electric field (V/m) distribution inside Cairo 500 substation during scenario 3.
0 50 100 150 200 250 300
0
50
100
150
200
250
300
350
400
0
5000
10000
15000
20000
25000
30000
35000
40000
45000
50000
55000
60000
65000
70000
75000
80000
85000
90000
95000
100000
105000
110000
0 50 100 150 200 250 300
0
50
100
150
200
250
300
350
400
-20000
0
20000
40000
60000
80000
100000
120000
140000
160000
180000
200000
220000
240000
260000
280000
300000
320000
340000
360000
380000
400000
 ISSN: 2252-8792
IJAPE Vol. 3, No. 2, August 2014 : 115 – 123
122
Table 2. The maximum and average electric field values for different working conditions.
Field
calculation
Height
Electric Field
Scenario
A (Standby
Off)
Scenario B
(Standby
On)
1.5 m
Et (Max) (kV/m) inside all
sub
21.98 23.5
Et (Max) (kV/m) inside 220
kV Switchyard
18.77 22.78
Et (Avg) (kV/m) 7.91 9.99
8.5 m
Et (Max) (kV/m) inside all
sub
103.35 129.99
Et (Max) (kV/m) inside 500
kV Switchyard
83.71 75.36
Et (Avg) (kV/m) 9.04 13.94
11 m
Et (Max) (kV/m) inside all
sub
123.34 158.55
Et (Max) (kV/m) inside 220
kV Switchyard
99.09 98.17
Et (Avg) (kV/m) 9.70 14.44
14 m
Et (Max) (kV/m) inside all
sub
127.73 135.69
Et (Avg) (kV/m) 10.97 14.38
17 m
Et (Max) (kV/m) inside all
sub
149.46 152.73
Et (Avg) (kV/m) 10.69 12.55
From these figures and table presented above, it is found that the maximum calculated electric field
imposed to the human body during hot-stick position (scenario 1) is about 23.5 kV/m while the maximum
measured electric field imposed to the human body during this position (scenario 1) is about 23 kV/m, and
the average calculated electric field imposed to the human body during hot-stick position (scenario 1) is
about 10 kV/m while the average measured electric field imposed to the human body during this position
(scenario 1) is about 9.6 kV/m. Therefore the simulation results are matched with the measured values with
very small tolerance (about 2.2%) which is because of the assumption taken during the simulation and due to
the field meter used in the measurements is dependent on the natural of place where the electric field is
measured [9- 11]. It is also found that the maximum calculated electric field imposed to the human body
during bare- hand position (scenario 2) is about 158.6 kV/m and that for scenario 3 is about 152.7 kV/m
(without considering the effects of insulating clothes) which are consistent with other related study [12].
Following the electric field during live line maintenance, the electric field intensity is higher,
exceeds, the exposure limit. So the workers should not last for more than several minutes in live line
maintenance position.
4. CONCLUSION
In this study, a method is proposed for determining the distribution of the electric field produced
inside high-voltage open distribution substations. This method is based on the charge simulation technique.
And the most important results from this study are as follows:
 It is found that the electric field changes from point to point inside substation switchyard.
According to this investigation results, a map of electric field intensity distribution was build for
this substation. This map depicts location of areas with different level electric field intensity. This
map is used for planning and conducting works inside substations and for moving inside
substation for equipment inspection.
 This investigation showed that, in average, about 42.3% of the open distribution substations
occupy the territory on which the electric field does not exceed 5 kV / m (zone of security), and
the maximum electric field intensity at this substation is less than 25 kV/m and only at certain
points in some open distribution substations reaches avalue greater than 25 kV/m.
IJAPE ISSN: 2252-8792 
Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution… (Essam M. Shaalan)
123
 The value of electric field during live line maintenance is higher, exceeds, the exposure limit. So
the workers should not last for more than several minutes in live line maintenance position.
REFERENCES
[1] L. Ortiz, J. Zoletti, F. Saavedra, A. Gonzales, “ELF Field Emissions from Electric Power Systems”, Proceedings of
the EMC 94, Roma, Italy, pp. 426-430, Sept. 1994.
[2] WHO - World Health Organization. “Extremely low frequency fields. Environmental Health Criteria”, World
Health Organization, Geneva, Vol. 238, 2007.
[3] "EMF Design Guidelines for Electric facilities", Report, Southern California Edison Company (SCE), Sept 2004.
[4] IEEE Std. Safety Levels With Respect to Human Exposure to Electromagnetic Fields, 0 to 3 kHz, IEEE Std.
C95.6-2002, Oct. 2002.
[5] N. H. Malik, "A Review of the Charge Simulation Method and Its Applications", IEEE Trans. On Electrical
Insulation, Vol. 24, No. 1, pp. 3-20, Feb. 1989.
[6] E.kuffel, W.S. Zaengle and J. Kuffel, “High voltage engineering, fundamentals”, Newnes, Second edition reprint,
2001 (Text book).
[7] Masanori Akazaki and Kiyoto Mishijima, “Calculation of three dimensional axisymmetric fields by charge
simulation method”, Electrical Engineering in Japan, vol. 98 no. 4, pp.1–7, July 1978.
[8] SanPiN 2.2.4.1191-03 Electromagnetic fields in the working environment, 16 October 2008.
[9] HI 3604 ELF Survey Meter User‟s Manual, Holladay Ind. 2002.
[10] HI-4413 Fiber Optic RS-232 Interface With Probe View™ 3600 User‟s manual, 2002.
[11] I.S. Okrainskaya, S.P. Gladyshev, A.I. Sidorov and N.V. Glotova, “Investigation of Electric Field Distribution
Inside 500 kV Power Distribution Substations”, 2013 IEEE International Conference on Electro Information
Technology (EIT), pp. 1 - 4, Rapid City, South Dakota, USA, 9-11 May 2013.
[12] W. Krajewski, “Numerical assessment of electromagnetic exposure during live-line works on high-voltage
objects”, Science Measurement & Technology IET, Volume: 3 , Issue 1, pp. 27-38, 2009.
BIOGRAPHIES OF AUTHORS
Sayed A. Ward was born in Cairo, Egypt, on December 24, 1961. He received the
B.Sc. degree in electrical engineering with honor in 1984 and the M.Sc. degree in high-
voltage Engineering in 1988, both from Zagazig University, Shoubra, Cairo, Egypt. He
received the Ph.D. degree in high-voltage engineering in 1992 from Cairo University.
He is currently Head of Electrical Engineering Department, Faculty of Engineering
(Shoubra), Cairo, Egypt. His research activity includes studying the gas discharge
phenomena in GIS, breakdown voltage study in GIS systems for compressed gases and
gas mixtures. Also his research activity includes breakdown in Insulating Oils and
DGA oil analysis in power transformers.
Samy M. Ghania was born in Egypt on December 28, 1971. He received the B.Sc.,
M.Sc., and Ph.D. degrees in electrical engineering from Shoubra Faculty of
Engineering, Zagazig University, Cairo, Egypt, in 1995, 2001, and 2005, respectively.
In July 2006, he joined the University of Waterloo, Waterloo, ON, Canada, as
Postdoctoral Fellow. He is currently an Ass. Professor at Electrical Engineering
Department, Faculty of Engineering (Shoubra), Cairo, Egypt. His areas of interest
include modelling and simulation of electrical machines, drives for electrical vehicles.
Essam M. Shaalan was born in Cairo, Egypt, on January 12, 1985. He received the
B.Sc. degree in electrical engineering with honor in 2007 from Benha University,
Shoubra, Cairo, Egypt. He received the M.Sc. degrees in electrical engineering from
Benha University, Shoubra, Cairo, Egypt. He is currently an Ass. Lecturer at Electrical
Engineering Department, Faculty of Engineering (Shoubra), Cairo, Egypt. His research
activity includes studying the high voltage electric fields and studing the effect of these
fields on human/workers.

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Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution Substations During Working Conditions

  • 1. International Journal of Applied Power Engineering (IJAPE) Vol. 3, No. 2, August 2014, pp. 115~123 ISSN: 2252-8792  115 Journal homepage: http://iaesjournal.com/online/index.php/IJAPE Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution Substations during Working Conditions Sayed A. Ward , Samy M. Ghania, Essam M. Shaalan Electrical Engineering Department, Faculty of Engineering at Shoubra Benha University, Cairo, Egypt Article Info ABSTRACT Article history: Received Mar 2, 2014 Revised Jul 10, 2014 Accepted Jul 23, 2014 The high level electric field intensity produced by high voltage (HV) equipments inside 500/220 kV substations is harmful for the human (staff) health. Therefore the minimum health and safety requirements regarding the exposure of workers to the risk arising from electric fields produced inside these substations is still considered as a competitive topic for utility designers, world health organization (WHO) and biomedical field researchers. It is very important to have knowledge about levels distribution of electric field intensity within these high voltage substations as early stage in the process of substation design. This paper presents results of investigation 50Hz electric field intensity distribution inside 500/220 kV power transmission substations in Cairo, Egypt. This paper presents a method for assessment the distribution of 50HZ electric field intensity distribution inside this substation, this method of analysis is based on the charge simulation technique (CSM). This study will serve for planning service works or for inspection of equipment on HV power transmission substations. Keyword: Charge simulation technique Electric field intensity High voltage substations Copyright © 2014 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Essam M. Shaalan, Electrical Engineering Department, Faculty of Engineering at Shoubra, Benha University, Cairo, Egypt e-mail: essam.shihata@feng.bu.edu.eg 1. INTRODUCTION Powerful electric systems with very high voltage are the source of harmful electromagnetic field radiation. This is because these electromagnetic field radiations represent the primary source to the resultant electrical current induced in the human body under or near electric power systems [1]. Therefore, the problem of the human exposure to electric fields has become more important with increasing the number and the size of power substations and electric power systems in general. This harmful attract an increased attention of many biomedical field researchers, scientific research communities worldwide on the health effects of electric power systems. As a result of this interest, the governments are playing an active role in the reduction of these exposures to electric fields by setting exposure limits for such fields which resulting from different electrical power systems [2-4], to guarantee the life insurance of all staff working inside these substations. The 50 Hz electromagnetic field is distributed unevenly in space between separate power installations inside HV substations. In open 500/220 kV power transmission substations, the sum of electromagnetic field sources with grounded metal constructions creates a complex picture of the electric field. Works are connected with operative switching, equipment inspection; different repair work, etc. require presence of staff personal in various points of 500kV & 220kV Switchyards (substation territory). Therefore, the investigation of the distribution levels of the electric fields inside these substations is an important step for solving the problem of personnel protection from the effects of these fields.
  • 2.  ISSN: 2252-8792 IJAPE Vol. 3, No. 2, August 2014 : 115 – 123 116 In this paper, the present algorithm is carried out to assessment the distribution levels of the electric field intensity produced by different high voltage electrical power systems inside 500/220 kV air-insulated substation (AIS). In addition to the investigation of levels distribution of electric field intensity inside 500/220 kV AIS at 1.5 m from ground surface, we will also investigate the distribution levels of electric field intensity during different working conditions and at different positions inside this substation. These calculated levels will be compared to the standard limit levels stated by international organizations [2-4]. This developed method is based on the charge simulation technique, which simulate the typical 500/220 kV substation with all incoming and outgoing feeders by developing multi-scripts of m-file Matlab software package to calculate the distribution levels of electric field intensity inside this substation. This method is considering the complex systems, including three-dimensional multiple incoming, outgoing overhead lines and bus system inside this substation. 2. SUBSTATION DESCRIPTION AND SYSTEM MODELING The calculations of electric fields are performed inside 500/220 kV AIS, Cairo 500 substation. This substation is supplied by four 500 kV overhead transmission lines, single circuit, which are connected to the same 500 kV double bus systems, main and standby bus-bars. This substation has three identical 3-ph, 500 MVA, 500/220/11 kV power transformers installed inside it, each one is composed of three single phase transformers. This substation is supplying six loads through six 220 kV double-circuit overhead transmission lines which are outgoing from the same 220 kV double bus systems, main and standby bus-bars. This substation has a simply 500 kV,220 kV bus systems with 300 m long and 12 m, 9m height respectively. Single line diagram for this substation is presented in Fig. 1. The location of equipment in the open distribution substation, as usual, is asymmetrical. Some equipment is often locates in separate groups. Between these equipments, there are a complex system of busbar, incoming and outgoing feeders which are similar to the web covering all open distribution substation. This complicates the task of investigation the fifty hertz electric field intensity. The human body is allocated within the highly exposure zones of electric fields inside this substation and at different heights to determine the field distribution levels during different working conditions, Fig. 2. Works are connected with operative switching, equipment inspection; different repair work, etc. require presence of staff personal in various points of 500kV & 220kV Switchyards (substation territory). Therefore, the investigation of the distribution levels of the electric fields inside these substations is carried out during different working conditions for staff. The first Scenario is carried out at a height of 1.5 m above the ground level which presents worker (staff) standing with his foot on ground inside switchyards during normal operation and (hot-stick position) during live- working conditions (Scenario 1). The second Scenario is carried out at a height of 11 m for 500 kV switchyard and 8.5 m for 220 kV switchyard, which presents the position of the worker (staff) in (bare hand position) during live maintenance conditions for 500 kV and 220 kV bus systems (Scenario 2). The third Scenario is carried out at a height of 17 m for 500 kV switchyard and 14 m for 220 kV switchyard, which presents the position of the worker (staff) in (bare hand position) during live maintenance conditions for 500 kV and 220 kV incoming and outgoing feeders (Scenario 3). In the electric field model presented in this paper, 500 kV bus-bars (HV bars) and 220 kV bus-bars (LV bars), incoming 500 kV feeders and outgoing 220 kV feeders are approximated by internally located line charges. Such a simplification is acceptable when the field is analyzed at a long enough distance from the conductor, e.g. near the ground surface. The electric potential of incoming 500 kV feeders, outgoing 220 kV feeders and bus-bar surfaces has been defined as complex potentials and assumed to be equal to their phase voltage. These assumptions lead to a charge simulation method formulation. The standby bus-bars are represented by line charges, their potential is assumed to be zero. The influence of tower insulators is neglected when the field is calculated. In this paper the HV systems of alternating current are considered, therefore the potential and charge densities are complex quantities. In this paper the Charge Simulation Method is used to compute the electric fields [5], where the live conductors are simulated by a number of discrete simulation charges located on the axis of these conductors. Values of simulation charges are determined by satisfying the boundary conditions at a number of contour points selected at the conductor surfaces. Once the values of simulation charges are determined, then the potential and electric field of any point in the region outside the conductors can be calculated using the superposition principle using the following equations:
  • 3. IJAPE ISSN: 2252-8792  Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution… (Essam M. Shaalan) 117 Figure 1. Single line diagram of simulated 500/220 kV AIS substation, Cairo 500 substation. ]][[][ QPV  (1) Where: [Q] is a column vector of the fictitious simulation charges, [V] is a column vector of the potential given by the boundary conditions and [P] is the matrix of the Maxwell potential coefficients which depend on the type of fictitious simulation charges [5, 6]. In our developed model, we simulate HV and LV bus-bars, incoming 500 kV feeders and outgoing 220 kV feeders by internally located line charges on their axes. Therefore the potential coefficient is given by [7]:          ))(( ))(( ln 4 1 221121 221121 dLLdLL dLLdLL d Pij  (2)
  • 4.  ISSN: 2252-8792 IJAPE Vol. 3, No. 2, August 2014 : 115 – 123 118 Where 2 1 2 1 2 11 )()()( ZZYYXXL  2 2 2 2 2 22 )()()( ZZYYXXL  2 1 2 1 2 111 )()()( ZZYYXXL  2 2 2 2 2 222 )()()( ZZYYXXL  2 21 2 21 2 21 )()()( ZZYYXXd  Figure 2. Different positions of the workers during different working conditions.                                                                  2)(1)( 4 1 2)(1)( 4 1 2)(1)( 4 1 22 2 11 1 2 2 1 1 22 2 11 1 2 2 1 1 22 2 11 1 2 2 1 1 L ZZ L ZZ L ZZ L ZZ d F L YY L YY L YY L YY d F L XX L XX L XX L XX d F z y x    (3) Where )( 1 )( 1 1 2121 dLLdLL     )( 1 )( 1 2 22112211 dLLdLL     Therefore the net field (Ei) at any point (Pi) due to a number of individual charges (n) each with charge of (Qj.) is given as:       z n j jzijy n j jyijx n j jxiji aQFaQFaQFE    111 *)(*)(*)( (4) Where (Fij)x, (Fij)y and (Fij)z are the „field intensity‟ or field coefficients and ax, ay and az are unit vectors in the x, y and z directions, respectively [7]. The total electric field at the ith contour point is expressed as:
  • 5. IJAPE ISSN: 2252-8792  Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution… (Essam M. Shaalan) 119 222 ( ziyixii EEEE  (5) 3. SIMULATION RESULTS AND DISCUSSIONS This study was conducted not only for a workers standing on the ground surface with his foot in switchyards during normal operation and (hot-stick position) during live- working conditions (Scenario 1), but also for a workers in live line maintenance position (bare hand position), at a height of 11 m for 500 kV switchyard and 8.5 m for 220 kV switchyard (Scenario 2) and at a height of 17 m for 500 kV switchyard and 14 m for 220 kV switchyard (Scenario 3). The human body was assumed to be standing in free space and not in contact with electrical ground. Workers in bare-hand working operate very close to live conductors and they wear special conductive clothing which protects them against the exposure of the electric field. These clothes are ignored in our simulation. The research results which are presented in this paper were carried out at the same actual schedule of working conditions for selected substation. These results have been presented in form of the electric field distribution maps and surface distribution (Fig. 3 & Fig. 4). The results of work are currently used for organization of the regular works on open distribution substations. Presentation of results in the form of maps, contours and three dimensional figures provides great visibility and a convenience in practical application. For example, when it is necessary to select a proper route for inspection substation or when choosing the proper protective equipment necessary for working personal without turned off above voltage, etc. Figure 3. Map of the electric field (V/m) distribution inside Cairo 500 substation during scenario 1. Table 1. The Distribution of Electric Field in the Zone of Open Distribution Substation (Scenario 1). 0 50 100 150 200 250 300 0 50 100 150 200 250 300 350 400 -1000 0 1000 2000 3000 4000 5000 6000 7000 8000 9000 10000 11000 12000 13000 14000 15000 16000 17000 18000 19000 20000 21000 22000 The part of the open distribution substation territory,%, where the electric field is in the range (E in kV/m) E Range 0≤Е<5 5≤Е<10 10≤Е<15 15≤E<20 20≤E<25 25≤E<30 Territory,%, 42.3 21.5 11.3 10.7 7 7.2
  • 6.  ISSN: 2252-8792 IJAPE Vol. 3, No. 2, August 2014 : 115 – 123 120 According to recommendations of SanPiN 2.2.4.1191-03 [8], employees, serving electrical installations are permitted to:  stay in the 50-HZ electric field with the intensity of up to 5 kV / m during the working day;  stay in the 50-HZ electric field with the intensity from 5 to 20 kV / m during limited time, calculated as follows: 2 50  E T (6) Where E is the electric field intensity in kV/m in the controlled area, T is the time in hrs. Therefore when the electric field intensity is in range from 20 to 25 kV/m, stay of the staff in this electric field should not exceed 10 minutes;  Maximal permitted level of the electric field intensity in open distribution substation is 25 kV / m.  Staying in the electric field with the intensity of more than 25 kV / m without use of the protective equipment is not permitted. Going along the calculated electric field intensity, it is determined the points where the electric field intensity reaches the maximum exposure limit values 5, 10, 15, 20 kV/m. Table 1 depicts, in percents, values of zones with electric field intensities less 5kV/m (zone of security) and higher 5kV/m (zone of influence) at scenario 1. Results of calculated data analysis in (Table 1) are showed that, in average; 42.3% of the open distribution substations occupy the territory on which the electric field does not exceed 5 kV / m (zone of security). And the territory of open distribution substations at which the electric field is greater than 5 kV / m, where it requires limited stay time for safety performance of work, is called the zone of electric field influence. This territory takes, in average, about 57.7% of the open distribution substation. The distribution of the electric field intensity in the zone of electric field influence where the electric field intensity higher 5kV/m is as follows:  21.5% of the territory falls on the zone with the electric field from 5 to 10 kV/m,  The zone from 10 kV to 15 kV/m is much smaller (about 11.3% of the territory of AIS).  The zone from 15 kV to 20 kV/m is about 10.7% of the territory of AIS.  The percentage of the zone with the intensity from 20 to 25 kV/m, where the permission stay time is not exceed 10 minutes, is about 7% of the territory of AIS.  The intensity of the electric field more than 25 kV/m, where the presence without personal protective equipment is prohibited, and the value of such zones is the about 7.2% of the territory of AIS. Figure 4. The electric field distribution (V/m) inside selected substation switchyard during scenario 1. Fig. 5 and Fig. 6 slow the electric field distribution inside Cairo 500 substation for the other two scenarios 2 & 3 mentioned previously, while Table 2 summarize the maximum and average electric field values for different working conditions.
  • 7. IJAPE ISSN: 2252-8792  Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution… (Essam M. Shaalan) 121 Figure 5. Map of the electric field (V/m) distribution inside Cairo 500 substation during scenario 2. Figure 6. Map of the electric field (V/m) distribution inside Cairo 500 substation during scenario 3. 0 50 100 150 200 250 300 0 50 100 150 200 250 300 350 400 0 5000 10000 15000 20000 25000 30000 35000 40000 45000 50000 55000 60000 65000 70000 75000 80000 85000 90000 95000 100000 105000 110000 0 50 100 150 200 250 300 0 50 100 150 200 250 300 350 400 -20000 0 20000 40000 60000 80000 100000 120000 140000 160000 180000 200000 220000 240000 260000 280000 300000 320000 340000 360000 380000 400000
  • 8.  ISSN: 2252-8792 IJAPE Vol. 3, No. 2, August 2014 : 115 – 123 122 Table 2. The maximum and average electric field values for different working conditions. Field calculation Height Electric Field Scenario A (Standby Off) Scenario B (Standby On) 1.5 m Et (Max) (kV/m) inside all sub 21.98 23.5 Et (Max) (kV/m) inside 220 kV Switchyard 18.77 22.78 Et (Avg) (kV/m) 7.91 9.99 8.5 m Et (Max) (kV/m) inside all sub 103.35 129.99 Et (Max) (kV/m) inside 500 kV Switchyard 83.71 75.36 Et (Avg) (kV/m) 9.04 13.94 11 m Et (Max) (kV/m) inside all sub 123.34 158.55 Et (Max) (kV/m) inside 220 kV Switchyard 99.09 98.17 Et (Avg) (kV/m) 9.70 14.44 14 m Et (Max) (kV/m) inside all sub 127.73 135.69 Et (Avg) (kV/m) 10.97 14.38 17 m Et (Max) (kV/m) inside all sub 149.46 152.73 Et (Avg) (kV/m) 10.69 12.55 From these figures and table presented above, it is found that the maximum calculated electric field imposed to the human body during hot-stick position (scenario 1) is about 23.5 kV/m while the maximum measured electric field imposed to the human body during this position (scenario 1) is about 23 kV/m, and the average calculated electric field imposed to the human body during hot-stick position (scenario 1) is about 10 kV/m while the average measured electric field imposed to the human body during this position (scenario 1) is about 9.6 kV/m. Therefore the simulation results are matched with the measured values with very small tolerance (about 2.2%) which is because of the assumption taken during the simulation and due to the field meter used in the measurements is dependent on the natural of place where the electric field is measured [9- 11]. It is also found that the maximum calculated electric field imposed to the human body during bare- hand position (scenario 2) is about 158.6 kV/m and that for scenario 3 is about 152.7 kV/m (without considering the effects of insulating clothes) which are consistent with other related study [12]. Following the electric field during live line maintenance, the electric field intensity is higher, exceeds, the exposure limit. So the workers should not last for more than several minutes in live line maintenance position. 4. CONCLUSION In this study, a method is proposed for determining the distribution of the electric field produced inside high-voltage open distribution substations. This method is based on the charge simulation technique. And the most important results from this study are as follows:  It is found that the electric field changes from point to point inside substation switchyard. According to this investigation results, a map of electric field intensity distribution was build for this substation. This map depicts location of areas with different level electric field intensity. This map is used for planning and conducting works inside substations and for moving inside substation for equipment inspection.  This investigation showed that, in average, about 42.3% of the open distribution substations occupy the territory on which the electric field does not exceed 5 kV / m (zone of security), and the maximum electric field intensity at this substation is less than 25 kV/m and only at certain points in some open distribution substations reaches avalue greater than 25 kV/m.
  • 9. IJAPE ISSN: 2252-8792  Assessment of Electric Field Distribution Inside 500/220 kV Open Distribution… (Essam M. Shaalan) 123  The value of electric field during live line maintenance is higher, exceeds, the exposure limit. So the workers should not last for more than several minutes in live line maintenance position. REFERENCES [1] L. Ortiz, J. Zoletti, F. Saavedra, A. Gonzales, “ELF Field Emissions from Electric Power Systems”, Proceedings of the EMC 94, Roma, Italy, pp. 426-430, Sept. 1994. [2] WHO - World Health Organization. “Extremely low frequency fields. Environmental Health Criteria”, World Health Organization, Geneva, Vol. 238, 2007. [3] "EMF Design Guidelines for Electric facilities", Report, Southern California Edison Company (SCE), Sept 2004. [4] IEEE Std. Safety Levels With Respect to Human Exposure to Electromagnetic Fields, 0 to 3 kHz, IEEE Std. C95.6-2002, Oct. 2002. [5] N. H. Malik, "A Review of the Charge Simulation Method and Its Applications", IEEE Trans. On Electrical Insulation, Vol. 24, No. 1, pp. 3-20, Feb. 1989. [6] E.kuffel, W.S. Zaengle and J. Kuffel, “High voltage engineering, fundamentals”, Newnes, Second edition reprint, 2001 (Text book). [7] Masanori Akazaki and Kiyoto Mishijima, “Calculation of three dimensional axisymmetric fields by charge simulation method”, Electrical Engineering in Japan, vol. 98 no. 4, pp.1–7, July 1978. [8] SanPiN 2.2.4.1191-03 Electromagnetic fields in the working environment, 16 October 2008. [9] HI 3604 ELF Survey Meter User‟s Manual, Holladay Ind. 2002. [10] HI-4413 Fiber Optic RS-232 Interface With Probe View™ 3600 User‟s manual, 2002. [11] I.S. Okrainskaya, S.P. Gladyshev, A.I. Sidorov and N.V. Glotova, “Investigation of Electric Field Distribution Inside 500 kV Power Distribution Substations”, 2013 IEEE International Conference on Electro Information Technology (EIT), pp. 1 - 4, Rapid City, South Dakota, USA, 9-11 May 2013. [12] W. Krajewski, “Numerical assessment of electromagnetic exposure during live-line works on high-voltage objects”, Science Measurement & Technology IET, Volume: 3 , Issue 1, pp. 27-38, 2009. BIOGRAPHIES OF AUTHORS Sayed A. Ward was born in Cairo, Egypt, on December 24, 1961. He received the B.Sc. degree in electrical engineering with honor in 1984 and the M.Sc. degree in high- voltage Engineering in 1988, both from Zagazig University, Shoubra, Cairo, Egypt. He received the Ph.D. degree in high-voltage engineering in 1992 from Cairo University. He is currently Head of Electrical Engineering Department, Faculty of Engineering (Shoubra), Cairo, Egypt. His research activity includes studying the gas discharge phenomena in GIS, breakdown voltage study in GIS systems for compressed gases and gas mixtures. Also his research activity includes breakdown in Insulating Oils and DGA oil analysis in power transformers. Samy M. Ghania was born in Egypt on December 28, 1971. He received the B.Sc., M.Sc., and Ph.D. degrees in electrical engineering from Shoubra Faculty of Engineering, Zagazig University, Cairo, Egypt, in 1995, 2001, and 2005, respectively. In July 2006, he joined the University of Waterloo, Waterloo, ON, Canada, as Postdoctoral Fellow. He is currently an Ass. Professor at Electrical Engineering Department, Faculty of Engineering (Shoubra), Cairo, Egypt. His areas of interest include modelling and simulation of electrical machines, drives for electrical vehicles. Essam M. Shaalan was born in Cairo, Egypt, on January 12, 1985. He received the B.Sc. degree in electrical engineering with honor in 2007 from Benha University, Shoubra, Cairo, Egypt. He received the M.Sc. degrees in electrical engineering from Benha University, Shoubra, Cairo, Egypt. He is currently an Ass. Lecturer at Electrical Engineering Department, Faculty of Engineering (Shoubra), Cairo, Egypt. His research activity includes studying the high voltage electric fields and studing the effect of these fields on human/workers.