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International Journal of Applied Power Engineering (IJAPE)
Vol. 3, No. 3, December 2014, pp. 175~189
ISSN: 2252-8792  175
Journal homepage: http://iaesjournal.com/online/index.php/IJAPE
Investigation of Electric Field Distribution Inside 500/220 kV
Transformation Substations during Different 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 Oct 10, 2014
Revised Nov 8, 2014
Accepted Nov 26, 2014
This study depicts the electric field distributions inside a typical 500/220 kV
open distribution substation under actual loading conditions and during
different working conditions, Hot-Stick position and Bar-Hand position. The
electric field is investigated for different workers heights of 1m, 1.5m and
1.8m above ground during normal working condition (Hot-Stick position)
inside this substation. This in addition to assessment of the electric field at a
height levels of 8m, 11m, 14m and 17m above ground as positions for live
line maintenance under 220 kV Busbars, 500 kV Busbars, 220 kV Incoming
and Outgoing feeders and 500 kV Incoming and Outgoing feeders
respectively. In this study the simulation results of the electric field obtained
using three dimensional (3D) computer model for existing typical high
voltage transformation substation are compared with field values measured
inside this typical substation and presented and discussed not only in the
form of contour maps but also in the form 3D surface and wireframe maps.
The simulation results are good matched and agreed with measured values.
This in addition to the electric field will be tabulated and compared to
international guidelines for personnel exposure to electric field. This study
will serve for planning service works or for inspection of equipment inside
high voltage (HV) power transformation substations.
Keyword:
Charge simulation technique
Electric field strength
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.
Email: essam.shihata@feng.bu.edu.eg
1. INTRODUCTION
For much of the history of the electrical power system, the size of a high voltage transmission
system was not of much concern because they were located in rural or heavily industrialized areas where the
cost of the real estate was small and their overbearing presence was of little concern to the general public.
Their exposure may be as small as walking under it or large as constructing a home or business under it.
The ever-increasing need for electrical energy has resulted in high voltage substations being placed much
closer to their loads and in commercial or residential areas. To exemplify this, consider that a high voltage
substation does not have a negative impact when it is constructed adjacent to a refinery or paper mill. In
addition to visual impact, there is ongoing concern about the effect of exposure to electric and magnetic
fields.
An area of little investigation until now is the electric fields generated by a transformation
substation and how these will change as we try to decrease the size and height of the substation. Constructing
a substation with a more compact design will result in increased electric field exposures to any workers in the
energized substation. As the workers cannot be exposed to a potentially unsafe amount of electric field, we
will have to balance the compact design with the amounts of electric field exposure.
 ISSN: 2252-8792
IJAPE Vol. 3, No. 3, December 2014 : 175 – 189
176
The effect of the electric field is especially important in the areas closed to high voltage facilities.
The electric field strength that occurs in the vicinity of these HV facilities must not exceed the levels
proposed by environmental and health regulations and standards [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 [2-6], to guarantee the life insurance of all staff working inside these substations.
Inside 500/220 kV substation, Works are connected with operative switching, equipment inspection,
different repair work, etc. require presence of staff personal in various points of 500 kV and 220kV
Switchyards (substation territory). Therefore, the investigation for 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.
In this study, 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
(AIS) substation. This study depicts the electric field distributions inside a typical 500/220 kV substation,
Cairo 500 substation, under actual loading conditions and during different working conditions (Hot-Stick
position and Bar-Hand position). The electric field is investigated for different workers heights of 1m, 1.5m
and 1.8m above ground. These fields are observed during normal working condition (Hot-Stick position)
inside this substation. This in addition to assessment of these fields at different height levels which represent
the possible positions of workers during working as live line maintenance (Bar-Hand position) such as at
heights of 8m, 11m, 14m and 17m above ground as positions for live line maintenance under 220 kV
Busbars, 500 kV Busbars, 220 kV Incoming and Outgoing feeders and 500 kV Incoming and Outgoing
feeders respectively. In this study the simulation results of the electric field obtained using three dimensional
(3D) computer model for existing typical substation are compared with field values measured inside this
typical substation and compared with international guidelines for personnel exposure to electric field [3, 4].
The results are tabulated and presented not only in the form of contour maps but also in the form 3D surface
and wireframe maps. This study will serve for planning service works or for inspection of equipment inside
HV power transformation substations.
2. SUBSTATION DESCRIPTION
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. 3D
spatial models of this substation, Cairo 500 substation, for all substation area, 500 kV switchyard and 220 kV
switchyard are presented in Figures 1, 2 and 3 respectively.
Figure 1. The 3D spatial model of Cairo 500 substation, all area.
IJAPE ISSN: 2252-8792 
Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan)
177
Figure 2. The 3D spatial model of Cairo 500 substation, 500 kV Switchyard
Figure 3. The 3D spatial model of Cairo 500 substation, 220 kV Switchyard.
3. SUBSTATION MODELING
In this study CSM is used to compute the electric field inside this substation produced by main
substation power conductors and sub conductors. The developed M-Scripts are using the discrete fictitious
finite line charges for modeling of line conductors and busbars conductors. The higher voltage (HV) 500 kV
bus conductors lower voltage (LV) 220 kV bus conductors, 500 kV incoming and outgoing feeders and 220
kV ingoing and outgoing feeders are approximated by internally located fictitious finite line charges along
the center axes of them. These line charges are considered as a proposed solution of Laplace equation which
governs the assessment of the electric field [7-10].
The electric potential of all incoming feeders, outgoing 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 finite line fictitious charges,
their potential is assumed to be zero. The electric field inside HV substations are excited by all conductors
under voltage and are deformed by metal, concrete, and ceramic (composite) elements such as tower trusses,
supporting constructions, and insulators. In the electric field model presented in this study, these elements
will be ignored and the influence of supporting insulators is neglected. Such a simplification is acceptable
when the field is analyzed at along enough distance from the conductor, e.g. near the ground surface.
For evaluating the electric field distribution inside HV Cairo 500 substation, we consider the area of
our calculations inside this substation as 300*400 m2
around and underneath busbars; 300 m along the
busbars length (lateral direction / X- direction), 400 m along the incoming and outgoing feeders length
(longitudinal direction / Y- direction). This area is consist of two sections, one of them has 300 m on lateral
direction and 165 m on longitudinal direction for 500 kV switchyard, the second has 300 m on lateral
direction and 235 m on longitudinal direction for 220 kV switchyard. Fig. 4 and Fig. 5 show a simple
graphical model of 500 kV switchyard to be simulated (arrangement of 500 kV busbars, vertical connectors,
incoming feeders to busbars and outgoing feeders to transformers), while a simple graphical model of 220 kV
switchyard to be simulated is simply presented in Fig. 6 and Fig. 7 (arrangement of 220 kV busbars, vertical
connectors, incoming feeders from transformers to busbars and outgoing feeders to loads).
 ISSN: 2252-8792
IJAPE Vol. 3, No. 3, December 2014 : 175 – 189
178
* Busbar height = 12 m
* Incoming or outgoing to TR.s feeders height = 18 m
* Vertical connector length = 6 m
* Considered Area: 300 m along bus-bars (Lateral direction)
165 m along the horizontal incoming and
outgoing feeders(Longitudinal direction)
Space between
INC. Feeders
Space between INC.
Feeders
phases
Incoming
Feeder-1
Incoming
Feeder-2
Incoming
Feeder-3
Incoming
Feeder-4
outgoing
To TR-1
outgoing
To TR-2
outgoing
To TR-3
Space between
OUT. Feeders
Space between OUT.
Feeders
phases
c b a
c b a
c b
a
c b a
Space between
Bus Phases
x
x
x
Conductor
Section
Conductor
Center Line
x
Finite Line Fictitious Charge
Contour Point
Check Point
Distribution of Fictitious Charges, Contour
Points and Check Points on the conductors
Figure 4. Developed model of 500 kV switchyard arrangement to be simulated.
4. ELECTRIC FIELD CALCULATION METHODOLOGY
In this paper the Charge Simulation Method is used to compute the electric fields. The basic
principle of CSM lies in replacing the surface charge of live conductors with a set of discrete fictitious finite
line
Figure 5. Graphical model of 500 kV switchyard arrangement to be simulated – 3D Spatial View.
Figure 6. Graphical model of 220 kV switchyard arrangement to be simulated – 3D Spatial View.
IJAPE ISSN: 2252-8792 
Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan)
179
Space between
OUT. Feeders
Space between
INC. Feeders
Space between INC.
Feeders phases
Incoming Feeder
From
TR-1
Outgoing
Feeder-2
2 Circuits
c b a
c b a
c b
a
Space between
Bus Phases
x
x
x
Conductor
Section
Conductor
Center Line
x
Finite Line Fictitious Charge
Contour Point
Check Point
Distribution of Fictitious Charges, Contour
Points and Check Points on the conductors
Incoming Feeder
From
TR-2
Incoming Feeder
From
TR-3
Space between OUT.
Feeders phases
* Busbar height = 9 m
* Incoming from TR.s or outgoing feeders height = 15 m
* Vertical connector length = 6 m
* Considered Area: 300 m along bus-bars (Lateral direction)
235 m along the horizontal incoming and
outgoing feeders(Longitudinal direction)
c b a
Outgoing
Feeder-1
2 Circuits
Outgoing
Feeder-3
2 Circuits
Outgoing
Feeder-4
2 Circuits
Outgoing
Feeder-5
2 Circuits
Outgoing
Feeder-6
2 Circuits
Figure 7. Developed model of 220 kV switchyard arrangement to be simulated
Charges, located inside the conductor and along the center axes of them, where these fictitious charges
generate the electric field of similar intensity and direction as the original conductors in the observed zone.
Figure. 8 shows a sample for the distribution of finite line charges, boundary points and check points on only
one phase conductor in developed models for simulation. These finite line charges and check points are
located at conductor levels while some contour points are located at conductor levels and others at ground
level to satisfy the image conditions. The values of these discrete charges are determined by satisfying the
boundary conditions in equation (1) at a selected number of contour points where the potentials of these
fictitious charges are taken as particular solutions of Laplace equation which governs the assessment of the
electric field [9, 10].
]][[][ 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,
[P] is the matrix of the Maxwell potential coefficients which depend on the type of fictitious simulation
charges as shown in fig. 9.
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:









))((
))((
ln
4
1
221121
221121
dLLdLL
dLLdLL
d
Pij

(2)
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 
 ISSN: 2252-8792
IJAPE Vol. 3, No. 3, December 2014 : 175 – 189
180



































































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)
x
x
x
Conductor
Section
Conductor
Center Line
x
Finite Line Fictitious Charge
Contour Point
Check Point
x
x x
x
x
x
x
Figure 8. Distribution of finite line charges, check and boundary points on only one phase.
X-axis
Z-axis
Y-axis
XX
Z
Z
Y
Y
P (X,Y, Z)
L
L
L
L
Q
Q
2
1
2
2
1
1
2
1
11
22
j
j
Figure 9. Finite line charge and contour point Pi in three dimensional x, y and z directions.
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 [10].
The total electric field at the ith
contour point is expressed as:
222
( ziyixii EEEE  (5)
IJAPE ISSN: 2252-8792 
Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan)
181
The methodology of 3D CSM used in the calculation and investigation of the electric field
distribution inside selected typical HV substation is simply presented in the schematic described in Figure.
10.
Figure 10. Simplified schematic diagram for the developed MATLAB program.
5. SIMULATION RESULTS AND DISCUSSIONS
5.1. Electric Field Distribution During Normal Conditions
The electric field is investigated inside a typical 500/220 kV substation under actual loading
conditions for different workers heights of 1m, 1.5m and 1.8m above ground during normal working
condition (Hot-Stick position) inside this substation. Figures 11, 12 and 13 present the electric field
distribution over all territory of selected substation for different workers heights of 1m, 1.5m and 1.8m above
ground in the form of contours maps respectively. From these figures, it is noticed that by increasing the
workers/calculation height, the density of electric fields' contour lines nearby the busbars, ingoing and
outgoing feeders increased and the maximum, average and minimum values of the electric field strength
increased also as shown in Table 1. This in adition to except for the areas nearby the busbars the contour
lines are aligned with the line conductors with electric field values related to the lines' voltage values.
Table 1. Electric field values for different workers heights of 1m, 1.5m and 1.8m inside HV 500/220 kV
substation.
Workers
/ Calc.
Height
Max Elec. Field Min. Elec. Field Avg.
Elec.
Field
(kV/m)
Value
(kV/m)
Position
(X, Y) m
Value
(V/m)
Position
(X, Y) m
1 m 24.23
x=220
y=300
71.92
x =0
y=137.5
8.49
1.5 m 25.78 76.53 9.04
1.8 m 27.11 80.47 9.5
 ISSN: 2252-8792
IJAPE Vol. 3, No. 3, December 2014 : 175 – 189
182
Figure 11. Contour map for the electric-field distribution throughout all the substation area, at 1m
above ground level.
Figure (12): Contour map for the electric-field distribution throughout all the substation area, at
1.5m above ground level
Figure 13. Contour map for the electric-field distribution throughout all the substation area, at 1.8m above
ground level.
0 50 100 150 200 250 300
Distance along Lateral Direction (m)
0
50
100
150
200
250
300
350
400
DistancealongLongitudinalDirection(m)
0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300
Distance along Lateral Direction (m)
0
20
40
60
80
100
120
140
160
180
200
220
240
260
280
300
320
340
360
380
400
420
DistancealongLongitudinalDirection(m)
0 50 100 150 200 250 300
Distance along Lateral Direction (m)
0
50
100
150
200
250
300
350
400
DistancealongLongitudinalDirection(m)
IJAPE ISSN: 2252-8792 
Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan)
183
These results obtained for electric field exposure entire all territory of the modeled substation are
analyzed and compared with international exposure limits and safety guidelines for electric field exposure for
the working personnel. Table (2) shows, in percent, values of zones entire all territory of this substation with
electric field intensities below and above international exposure limits and safety guidelines for electric field
exposure for different workers heights of 1m, 1.5m and 1.8m. While Table (3) and Table (4) show the
distribution of Electric Field strength over all territory of 220 kV and 500 kV switchyards area for different
workers heights of 1m, 1.5m and 1.8m respectively.
Table 2. Zones entire all territory of Cairo 500 substation with electric field below and above international
exposure limits for different workers heights, 1m, 1.5m and 1.8m.
ERange(kV/m)
ElectricfieldbelowPublicexposurelimit
(0≤Е<5)
ElectricfieldbelowICNIRPoccupational
exposurelimit
(5≤Е<10)
ElectricfieldaboveICNIRPoccupational
exposurelimitorbelowIEEEoccupational
exposurelimit
(10≤Е<20)
ElectricfieldaboveICNIRPorIEEE
occupationalexposurelimit
(E>20)
Territory,%,
For workers of
height 1m
45.5% 23.81% 28.07% 2.62%
Territory,%,
For workers of
height 1.5m
43.39% 23.99% 27.42% 5.20%
Territory,%,
For workers of
height 1.8m
42.03% 23.57% 25.97% 8.43%
Table 3. The distribution of Electric Field strength over all territory of 220 kV switchyard area for different
workers heights.
The part of 220 kV switchyard territory,%, where the
electric field is in the range (E in kV/m)
ERange
(kV/m)
0≤Е<5
5≤Е<10
10≤Е<15
Territory,%,
For workers of height 1m
76.7% 23.3% 0%
Territory,%,
For workers of height 1.5m
72.29% 25.32% 2.39%
Territory,%,
For workers of height 1.8m
71.56% 24.03% 4.29%
 ISSN: 2252-8792
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184
Table (4): The distribution of Electric Field strength over all territory of 500 kV switchyard area for different
workers heights.
The part of 500 kV switchyard 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,%, For
workers of height
1m
24.81
32.54
14.71
21.76
6.18
0
Territory,%,
For workers of
height 1.5m
22.56
31.68
15.81
18.35
11.14
0.46
Territory,%,
For workers of
height 1.8m 20.37
30.35
16.39
15.41
15.58
1.9
According to all investigations achieved above for different workers heights during working in live
condition at normal operation, the maximum values of the electric field strength obtained at most territory of
this substation are less than 20 kV/m (the guidelines of the IEEE Std. C95.6 for occupational exposure)
except only at certain few points (not exceeds 2.62% for workers of 1m height, 5.2% for workers of 1.5m
height and 8.43% for workers of 1.8m height of overall substation territory) in this substation it reaches and
exceeds 20 kV/m. These results are good matched and agreed with other related studies [11-13].
5.2. Electric Field Distribution During Live Line Maintenance
This study was conducted not only for a workers standing on the ground surface with his foot in
switchyards during normal operation (hot-stick position), but also for a workers in live line maintenance
position (bare hand position) under actual loading conditions. This field is calculated inside this modeled
typical HV substation at a height levels of 8m, 11m, 14m and 17m above ground, approximating the height
level of a workman above ground level during live line maintenance, as positions for live line working
condition inside this substation nearby and underneath 220 kV busbars, 500 kV busbars, 220 kV ingoing and
outgoing feeders and 500 kV ingoing and outgoing feeders respectively. This field is calculated without
considering the effects of insulating/protective clothes. Figures 14-a, 14-b, 15-a, 15-b, 16-a, 16-b, 17-a and
17-b present the electric field distribution over all territory of 500 kV and 220 kV switchyards at live line
maintenance height levels described previously in the form of contours map and 3D surface map respectively.
From these figures, it is noticed that the maximum electric field values imposed to the human body
during bare-hand position are 64.99 kV/m for height of 8m and occurs at position (x=210 m and y=90 m)
located under 220 kV Bus-2, 134.02 kV/m for height of 11m and occurs at position (x=288 m and y=345 m)
located under 500 kV Bus-1, 200.62 kV/m for height of 14m and occurs at position (x=60 m and y=75 m)
located underneath 220 kV Buses and 214.89 kV/m for height of 17m and occurs at position (x=66 m and
y=295 m) located under 500 kV Bus-1. According to all investigations achieved above for all cases and
positions of workers during working in live line maintenance, the maximum values of the electric field
strength obtained are good matched and consistent with other related studies [14,15].
IJAPE ISSN: 2252-8792 
Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan)
185
Figure 14. a. Contour map for the electric-field
strength distribution throughout 220 kV
switchyard area, at 8m above ground level.
Figure 14.B. Surface map for the electric-field strength
distribution throughout 220 kV switchyard area, at 8m
above ground level.
Figure (15-a): Contour map for the electric-field
strength distribution throughout 500 kV
switchyard area, at 11m above ground level.
Figure (15-b): Surface map for the electric-field
strength distribution throughout 500 kV switchyard
area, at 11m above ground level.
Figure 16.a. Contour map for the electric-field
strength distribution throughout 220 kV switchyard
area, at 14m above ground level.
Figure 16.b. Surface map for the electric-field
strength distribution throughout 220 kV switchyard
area, at 14m above ground level
0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300
Distance along Lateral Direction (m)
0
20
40
60
80
100
120
140
160
180
200
220
DistancealongLongitudinalDirection(m)
0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300
Distance along Lateral Direction (m)
240
260
280
300
320
340
360
380
400
DistancealongLongitudinalDirection(m)
0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300
Distance along Lateral Direction (m)
0
20
40
60
80
100
120
140
160
180
200
220
DistancealongLongitudinalDirection(m)
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IJAPE Vol. 3, No. 3, December 2014 : 175 – 189
186
Figure 17.a. Contour map for the electric-field
strength distribution throughout 500 kV switchyard
area, at 17m above ground level.
Figure (17-b): Surface map for the electric-field
strength distribution throughout 500 kV switchyard
area, at 17m above ground level.
6. MEASUREMENTS RESULTS AND DISCUSSIONS
The electric field produced inside this typical 500/220 kV substation is measured and profiled at a
longitudinal distances along 500kV and 220kV ingoing and outgoing lines, while it has been measured at a
lateral distances, along 500kV and 220kV bus bars. During these measurements, the electric sensor module
(HI 3604 ELF Survey Meter) should be placed far away from the human on a wooden tripod base unit, such
that the human body interference on the electric field measurements is avoided, and a fiber optic cable is used
to connect it to the base unit [16, 17]. The methodology of electric field measurements under buses and lines
conductors was conducted at a height of 1.5m above the ground to study the field levels experienced by
human beings through 301 measurement points under each phase of buses' conductors, 76 measurement
points under each phase of 500 kV incoming feeders' conductors, 91 measurement points under each phase of
500 kV outgoing feeders' conductors, 161 measurement points under each phase of 220 kV incoming feeders'
conductors and 71 measurement points under each phase of 220 kV outgoing feeders' conductors. Figures 18,
19, 20 and 21 show the longitudinal electric field profiles measured and calculated along 500kV and 220kV
bus bars and along 500kV outgoings and 220kV ingoings respectively.
These measurements showed that the electric field strength values are higher than the safe
occupational exposure limits at certain positions inside this substation. Table (5) shows the maximum
measured and calculated electric field strength values along all buses and feeders mentioned above. From
these tables, it is observed that the simulation results are consistent with the measured values with very small
tolerance 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.
Table 5. Maximum measured and calculated electric field values along all buses and feeders of Cairo 500
substation at height of 1.5m
Location
Max.
Measured
Elec. Field
(kV/m)
Max.
Calculated
Elec. Field
(kV/m)
Error,
%
Along 500 kV Buses 24.7 25.6 3.6%
Along 500 kV INC.s 16.68 16.23 2.7%
Along 500 kV OUT.s 16.66 16.82 0.96%
Along 220 kV Buses 10.56 11 4.2%
Along 220 kV INC.s 10.51 10.17 3.2%
Along 220 kV OUT.s 10.44 9.97 4.5%
0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300
Distance along Lateral Direction (m)
240
260
280
300
320
340
360
380
400
DistancealongLongitudinalDirection(m)
IJAPE ISSN: 2252-8792 
Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan)
187
Figure 18. Longitudinal electric field profiles measured and calculated along 500kV Buses inside Cairo 500
Substation.
Figure 19. Longitudinal electric field profiles measured and calculated along 220kV Buses inside Cairo 500
Substation.
Figure 20. Longitudinal electric field profiles measured and calculated along 500kV OUT.s inside Cairo 500
Substation.
0 50 100 150 200 250 300
0
0.5
1
1.5
2
2.5
3
x 10
4
Distance along Bus Length X(m)
TotalElectricFieldintensityE(V/m)
Total Electric Field Profile along 500kV Buses- Calculated Vs Measured at height of 1.5m
Cal. Field along Bus-1 (Y=350)
Meas. Field along Bus-1 (Y=350)
Cal. Field along Bus-2 (Y=300)
Meas. Field along Bus-2 (Y=300)
0 50 100 150 200 250 300
0
2000
4000
6000
8000
10000
12000
Distance along Bus Length X(m)
TotalElectricFieldintensityE(V/m)
Total Electric Field Profile along 220kV Buses- Calculated Vs Measured at height of 1.5m
Cal. Field along Bus-1 (Y=50)
Meas. Field along Bus-1 (Y=50)
Cal. Field along Bus-2 (Y=90)
Meas. Field along Bus-2 (Y=90)
230 240 250 260 270 280 290 300 310 320 330
0
2000
4000
6000
8000
10000
12000
14000
16000
18000
Distance along outgoing Length Y(m)
TotalElectricFieldintensityE(V/m)
Total Electric Field Profile along 500kV out Feeders- Calculated Vs Measured at height of 1.5m
Cal. Field along outgoing-1 (X=75)
Meas. Field along outgoing-1 (X=75)
Cal. Field along outgoing-2 (X=150)
Meas. Field along outgoing-2 (X=150)
Cal. Field along outgoing-3 (X=225)
Meas. Field along outgoing-3 (X=225)
 ISSN: 2252-8792
IJAPE Vol. 3, No. 3, December 2014 : 175 – 189
188
Figure 21 Longitudinal electric field profiles measured and calculated along 220kV INC.s inside Cairo 500
Substation.
7. CONCLUSIONS AND RECOMMENDATIONS
In this study, a method is proposed for investigation the distribution of the electric field produced
inside HV substations. This method is based on the charge simulation technique and the most important
results from this study are as follows:
 During working in live condition at normal operation inside 500/220 kV substations (hot-
stick position), the maximum values of the electric field strength at most territory of this substation
are less than 20 kV/m (the guidelines of the IEEE Std. C95.6 for occupational exposure) except only
at certain few points (not exceeds 2.62% for workers of 1m height, 5.2% for workers of 1.5m height
and 8.43% for workers of 1.8m height of overall substation territory) it exceeds 20 kV/m.
 By increasing the workers/calculation height, the density of electric fields nearby and underneath
busbars, ingoing and outgoing feeders increased and the area of zone of security (E<5 kV/m) entire
territory of modelled substation decreased while the area of zone of influence (E>5 kV/m)
increased.
 During working in live condition as live line maintenance inside 500/220 kV substations (Bar-hand
position), the values of the electric field strength are more danger while its maximum values exceed
25 kV/m with about 8.6 times, where the presence without personal protective equipment is much
prohibited.
 All simulation results are good matched and consistent with measurements results and other related
studies.
 It is recommended for using this study for planning service works or for inspection of equipment
inside high voltage power transformation substations.
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, Vol. 238.
Geneva, 2007.
[3] IEEE Std. Safety Levels With Respect to Human Exposure to Electromagnetic Fields, 0 to 3 kHz, IEEE Std.
C95.6-2002, Oct. 2002.
[4] International Commission on Non-Ionizing Radiation Protection (ICNIRP), Guidelines for limiting exposure to
time-varying electric and magnetic fields (1 Hz to 100 kHz), Vol. 99, No. 6, 818-836 Health Physics, 2010.
[5] National Radiological Protection Board (NRPB), Advice on limiting exposure to electromagnetic fields (0-300
GHz), Vol. 15, No. 2, 2004.
[6] "Directive 2004/40/EC of the European Parliament and of the Council of 29th April 2004 on “the minimum health
and safety requirements regarding the exposure of workers to the risk arising from physical agents (electromagnetic
fields)” (18th
individual Directive within the meaning of Article 16(1) of Directive 89/391/EEC)‟, Official Journal .
[7] H. Singer, H. Steinbigler, P. Weiss, "A Charge Simulation Method for the Calculation of High Voltage Fields",
IEEE Trans. on PAS, Vol. 93, P-P: 1660-1667, 1974.
[8] E.kuffel, W.S. Zaengle and J. Kuffel, “High Voltage Engineering, Fundamentals”, Second edition reprint, 2001
(Text book).
60 80 100 120 140 160 180 200 220 240
0
2000
4000
6000
8000
10000
12000
Distance along Incoming Length Y(m)
TotalElectricFieldintensityE(V/m)
Total Electric Field Profile along 220kV INC Feeders- Calculated Vs Measured at height of 1.5m
Cal. Field along Incoming-1 (X=56.25)
Meas. Field along Incoming-1 (X=56.25)
Cal. Field along Incoming-2 (X=150)
Meas. Field along Incoming-2 (X=150)
Cal. Field along Incoming-3 (X=243.75)
Meas. Field along Incoming-3 (X=243.75)
IJAPE ISSN: 2252-8792 
Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan)
189
[9] Nazar H. Malik, “A review of the Charge Simulation Method and its Applications” IEEE Transactions on
Electrical Insulation, Vol. 24, No. 1, P-P: 3–20, February 1989.
[10] 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.
[11] I.S. Okrainskaya, S.P. Gladyshev, A.I. SidorovAnd N.V. Glotova, “Investigation of Electric Field Distribution
Inside 500 kV Power Distribution Substations”, IEEE International Conference on Electro/ Information
Technology (EIT), P-P: 1 – 4, Rapid City, SD, 9-11 May 2013.
[12] I. S. Okrainskaya, A. V. Babin, A. I. Sidorov, et al., “General Characteristic of Electric Field Intensity of 500 kV
Outdoor Switchgears”, Power Technology and Engineering, Vol. 40, No. 2, P-P: 45 – 48, 2006. Translated from
Élektricheskie Stantsii, No. 1, January 2006.
[13] A.S. Safigianni, A.I. Spyridopoulos and V.L. Kanas, “Electric and Magnetic Field Measurements in a High
Voltage Center”, Ann. British Occupational Hygiene Society, Vol. 56, No. 1, P-P: 18–24, 2012.
[14] Samy M. Ghania, “Evaluation of Electromagnetic Fields Exposure during Live Line Working Conditions Inside
High Voltage Substations”, IRACST - Engineering Science and Technology: An International Journal (ESTIJ),
ISSN: 2250-3498, Vol. 3, No. 1, P-P: 199 – 206, February 2013.
[15] 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.
[16] HI 3604 ELF Survey Meter User‟s Manual, Holladay Ind. 2002.
[17] HI-4413 Fiber Optic RS-232 Interface With Probe View™ 3600 User‟s manual, 2002
BIOGRAPHIES OF AUTHORS
Sayed Abo-Elsood S. Ward: 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, faculty of engineering
(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 Mohamed A. Ghania: Ghania was born in Egypt on December 28, 1971. He received the
B.Sc., M.Sc., and Ph.D. degrees in electrical engineering from Faculty of Engineering (Shoubra),
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 modeling and simulation of electrical machines, drives for
electrical vehicles, studying the human exposure to high voltage electromagnetic fields.
Essam Mohamed A. Shaalan: 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,
Faculty of Engineering (Shoubra), Cairo, Egypt. He received the M.Sc. degrees in electrical
engineering from Benha University, Faculty of Engineering (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 studying the effect of these fields on human/workers.

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Investigation of Electric Field Distribution Inside 500/220 kV Transformation Substations during Different Working Conditions

  • 1. International Journal of Applied Power Engineering (IJAPE) Vol. 3, No. 3, December 2014, pp. 175~189 ISSN: 2252-8792  175 Journal homepage: http://iaesjournal.com/online/index.php/IJAPE Investigation of Electric Field Distribution Inside 500/220 kV Transformation Substations during Different 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 Oct 10, 2014 Revised Nov 8, 2014 Accepted Nov 26, 2014 This study depicts the electric field distributions inside a typical 500/220 kV open distribution substation under actual loading conditions and during different working conditions, Hot-Stick position and Bar-Hand position. The electric field is investigated for different workers heights of 1m, 1.5m and 1.8m above ground during normal working condition (Hot-Stick position) inside this substation. This in addition to assessment of the electric field at a height levels of 8m, 11m, 14m and 17m above ground as positions for live line maintenance under 220 kV Busbars, 500 kV Busbars, 220 kV Incoming and Outgoing feeders and 500 kV Incoming and Outgoing feeders respectively. In this study the simulation results of the electric field obtained using three dimensional (3D) computer model for existing typical high voltage transformation substation are compared with field values measured inside this typical substation and presented and discussed not only in the form of contour maps but also in the form 3D surface and wireframe maps. The simulation results are good matched and agreed with measured values. This in addition to the electric field will be tabulated and compared to international guidelines for personnel exposure to electric field. This study will serve for planning service works or for inspection of equipment inside high voltage (HV) power transformation substations. Keyword: Charge simulation technique Electric field strength 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. Email: essam.shihata@feng.bu.edu.eg 1. INTRODUCTION For much of the history of the electrical power system, the size of a high voltage transmission system was not of much concern because they were located in rural or heavily industrialized areas where the cost of the real estate was small and their overbearing presence was of little concern to the general public. Their exposure may be as small as walking under it or large as constructing a home or business under it. The ever-increasing need for electrical energy has resulted in high voltage substations being placed much closer to their loads and in commercial or residential areas. To exemplify this, consider that a high voltage substation does not have a negative impact when it is constructed adjacent to a refinery or paper mill. In addition to visual impact, there is ongoing concern about the effect of exposure to electric and magnetic fields. An area of little investigation until now is the electric fields generated by a transformation substation and how these will change as we try to decrease the size and height of the substation. Constructing a substation with a more compact design will result in increased electric field exposures to any workers in the energized substation. As the workers cannot be exposed to a potentially unsafe amount of electric field, we will have to balance the compact design with the amounts of electric field exposure.
  • 2.  ISSN: 2252-8792 IJAPE Vol. 3, No. 3, December 2014 : 175 – 189 176 The effect of the electric field is especially important in the areas closed to high voltage facilities. The electric field strength that occurs in the vicinity of these HV facilities must not exceed the levels proposed by environmental and health regulations and standards [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 [2-6], to guarantee the life insurance of all staff working inside these substations. Inside 500/220 kV substation, Works are connected with operative switching, equipment inspection, different repair work, etc. require presence of staff personal in various points of 500 kV and 220kV Switchyards (substation territory). Therefore, the investigation for 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. In this study, 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 (AIS) substation. This study depicts the electric field distributions inside a typical 500/220 kV substation, Cairo 500 substation, under actual loading conditions and during different working conditions (Hot-Stick position and Bar-Hand position). The electric field is investigated for different workers heights of 1m, 1.5m and 1.8m above ground. These fields are observed during normal working condition (Hot-Stick position) inside this substation. This in addition to assessment of these fields at different height levels which represent the possible positions of workers during working as live line maintenance (Bar-Hand position) such as at heights of 8m, 11m, 14m and 17m above ground as positions for live line maintenance under 220 kV Busbars, 500 kV Busbars, 220 kV Incoming and Outgoing feeders and 500 kV Incoming and Outgoing feeders respectively. In this study the simulation results of the electric field obtained using three dimensional (3D) computer model for existing typical substation are compared with field values measured inside this typical substation and compared with international guidelines for personnel exposure to electric field [3, 4]. The results are tabulated and presented not only in the form of contour maps but also in the form 3D surface and wireframe maps. This study will serve for planning service works or for inspection of equipment inside HV power transformation substations. 2. SUBSTATION DESCRIPTION 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. 3D spatial models of this substation, Cairo 500 substation, for all substation area, 500 kV switchyard and 220 kV switchyard are presented in Figures 1, 2 and 3 respectively. Figure 1. The 3D spatial model of Cairo 500 substation, all area.
  • 3. IJAPE ISSN: 2252-8792  Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan) 177 Figure 2. The 3D spatial model of Cairo 500 substation, 500 kV Switchyard Figure 3. The 3D spatial model of Cairo 500 substation, 220 kV Switchyard. 3. SUBSTATION MODELING In this study CSM is used to compute the electric field inside this substation produced by main substation power conductors and sub conductors. The developed M-Scripts are using the discrete fictitious finite line charges for modeling of line conductors and busbars conductors. The higher voltage (HV) 500 kV bus conductors lower voltage (LV) 220 kV bus conductors, 500 kV incoming and outgoing feeders and 220 kV ingoing and outgoing feeders are approximated by internally located fictitious finite line charges along the center axes of them. These line charges are considered as a proposed solution of Laplace equation which governs the assessment of the electric field [7-10]. The electric potential of all incoming feeders, outgoing 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 finite line fictitious charges, their potential is assumed to be zero. The electric field inside HV substations are excited by all conductors under voltage and are deformed by metal, concrete, and ceramic (composite) elements such as tower trusses, supporting constructions, and insulators. In the electric field model presented in this study, these elements will be ignored and the influence of supporting insulators is neglected. Such a simplification is acceptable when the field is analyzed at along enough distance from the conductor, e.g. near the ground surface. For evaluating the electric field distribution inside HV Cairo 500 substation, we consider the area of our calculations inside this substation as 300*400 m2 around and underneath busbars; 300 m along the busbars length (lateral direction / X- direction), 400 m along the incoming and outgoing feeders length (longitudinal direction / Y- direction). This area is consist of two sections, one of them has 300 m on lateral direction and 165 m on longitudinal direction for 500 kV switchyard, the second has 300 m on lateral direction and 235 m on longitudinal direction for 220 kV switchyard. Fig. 4 and Fig. 5 show a simple graphical model of 500 kV switchyard to be simulated (arrangement of 500 kV busbars, vertical connectors, incoming feeders to busbars and outgoing feeders to transformers), while a simple graphical model of 220 kV switchyard to be simulated is simply presented in Fig. 6 and Fig. 7 (arrangement of 220 kV busbars, vertical connectors, incoming feeders from transformers to busbars and outgoing feeders to loads).
  • 4.  ISSN: 2252-8792 IJAPE Vol. 3, No. 3, December 2014 : 175 – 189 178 * Busbar height = 12 m * Incoming or outgoing to TR.s feeders height = 18 m * Vertical connector length = 6 m * Considered Area: 300 m along bus-bars (Lateral direction) 165 m along the horizontal incoming and outgoing feeders(Longitudinal direction) Space between INC. Feeders Space between INC. Feeders phases Incoming Feeder-1 Incoming Feeder-2 Incoming Feeder-3 Incoming Feeder-4 outgoing To TR-1 outgoing To TR-2 outgoing To TR-3 Space between OUT. Feeders Space between OUT. Feeders phases c b a c b a c b a c b a Space between Bus Phases x x x Conductor Section Conductor Center Line x Finite Line Fictitious Charge Contour Point Check Point Distribution of Fictitious Charges, Contour Points and Check Points on the conductors Figure 4. Developed model of 500 kV switchyard arrangement to be simulated. 4. ELECTRIC FIELD CALCULATION METHODOLOGY In this paper the Charge Simulation Method is used to compute the electric fields. The basic principle of CSM lies in replacing the surface charge of live conductors with a set of discrete fictitious finite line Figure 5. Graphical model of 500 kV switchyard arrangement to be simulated – 3D Spatial View. Figure 6. Graphical model of 220 kV switchyard arrangement to be simulated – 3D Spatial View.
  • 5. IJAPE ISSN: 2252-8792  Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan) 179 Space between OUT. Feeders Space between INC. Feeders Space between INC. Feeders phases Incoming Feeder From TR-1 Outgoing Feeder-2 2 Circuits c b a c b a c b a Space between Bus Phases x x x Conductor Section Conductor Center Line x Finite Line Fictitious Charge Contour Point Check Point Distribution of Fictitious Charges, Contour Points and Check Points on the conductors Incoming Feeder From TR-2 Incoming Feeder From TR-3 Space between OUT. Feeders phases * Busbar height = 9 m * Incoming from TR.s or outgoing feeders height = 15 m * Vertical connector length = 6 m * Considered Area: 300 m along bus-bars (Lateral direction) 235 m along the horizontal incoming and outgoing feeders(Longitudinal direction) c b a Outgoing Feeder-1 2 Circuits Outgoing Feeder-3 2 Circuits Outgoing Feeder-4 2 Circuits Outgoing Feeder-5 2 Circuits Outgoing Feeder-6 2 Circuits Figure 7. Developed model of 220 kV switchyard arrangement to be simulated Charges, located inside the conductor and along the center axes of them, where these fictitious charges generate the electric field of similar intensity and direction as the original conductors in the observed zone. Figure. 8 shows a sample for the distribution of finite line charges, boundary points and check points on only one phase conductor in developed models for simulation. These finite line charges and check points are located at conductor levels while some contour points are located at conductor levels and others at ground level to satisfy the image conditions. The values of these discrete charges are determined by satisfying the boundary conditions in equation (1) at a selected number of contour points where the potentials of these fictitious charges are taken as particular solutions of Laplace equation which governs the assessment of the electric field [9, 10]. ]][[][ 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, [P] is the matrix of the Maxwell potential coefficients which depend on the type of fictitious simulation charges as shown in fig. 9. 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:          ))(( ))(( ln 4 1 221121 221121 dLLdLL dLLdLL d Pij  (2) 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 
  • 6.  ISSN: 2252-8792 IJAPE Vol. 3, No. 3, December 2014 : 175 – 189 180                                                                    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) x x x Conductor Section Conductor Center Line x Finite Line Fictitious Charge Contour Point Check Point x x x x x x x Figure 8. Distribution of finite line charges, check and boundary points on only one phase. X-axis Z-axis Y-axis XX Z Z Y Y P (X,Y, Z) L L L L Q Q 2 1 2 2 1 1 2 1 11 22 j j Figure 9. Finite line charge and contour point Pi in three dimensional x, y and z directions. 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 [10]. The total electric field at the ith contour point is expressed as: 222 ( ziyixii EEEE  (5)
  • 7. IJAPE ISSN: 2252-8792  Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan) 181 The methodology of 3D CSM used in the calculation and investigation of the electric field distribution inside selected typical HV substation is simply presented in the schematic described in Figure. 10. Figure 10. Simplified schematic diagram for the developed MATLAB program. 5. SIMULATION RESULTS AND DISCUSSIONS 5.1. Electric Field Distribution During Normal Conditions The electric field is investigated inside a typical 500/220 kV substation under actual loading conditions for different workers heights of 1m, 1.5m and 1.8m above ground during normal working condition (Hot-Stick position) inside this substation. Figures 11, 12 and 13 present the electric field distribution over all territory of selected substation for different workers heights of 1m, 1.5m and 1.8m above ground in the form of contours maps respectively. From these figures, it is noticed that by increasing the workers/calculation height, the density of electric fields' contour lines nearby the busbars, ingoing and outgoing feeders increased and the maximum, average and minimum values of the electric field strength increased also as shown in Table 1. This in adition to except for the areas nearby the busbars the contour lines are aligned with the line conductors with electric field values related to the lines' voltage values. Table 1. Electric field values for different workers heights of 1m, 1.5m and 1.8m inside HV 500/220 kV substation. Workers / Calc. Height Max Elec. Field Min. Elec. Field Avg. Elec. Field (kV/m) Value (kV/m) Position (X, Y) m Value (V/m) Position (X, Y) m 1 m 24.23 x=220 y=300 71.92 x =0 y=137.5 8.49 1.5 m 25.78 76.53 9.04 1.8 m 27.11 80.47 9.5
  • 8.  ISSN: 2252-8792 IJAPE Vol. 3, No. 3, December 2014 : 175 – 189 182 Figure 11. Contour map for the electric-field distribution throughout all the substation area, at 1m above ground level. Figure (12): Contour map for the electric-field distribution throughout all the substation area, at 1.5m above ground level Figure 13. Contour map for the electric-field distribution throughout all the substation area, at 1.8m above ground level. 0 50 100 150 200 250 300 Distance along Lateral Direction (m) 0 50 100 150 200 250 300 350 400 DistancealongLongitudinalDirection(m) 0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 Distance along Lateral Direction (m) 0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 380 400 420 DistancealongLongitudinalDirection(m) 0 50 100 150 200 250 300 Distance along Lateral Direction (m) 0 50 100 150 200 250 300 350 400 DistancealongLongitudinalDirection(m)
  • 9. IJAPE ISSN: 2252-8792  Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan) 183 These results obtained for electric field exposure entire all territory of the modeled substation are analyzed and compared with international exposure limits and safety guidelines for electric field exposure for the working personnel. Table (2) shows, in percent, values of zones entire all territory of this substation with electric field intensities below and above international exposure limits and safety guidelines for electric field exposure for different workers heights of 1m, 1.5m and 1.8m. While Table (3) and Table (4) show the distribution of Electric Field strength over all territory of 220 kV and 500 kV switchyards area for different workers heights of 1m, 1.5m and 1.8m respectively. Table 2. Zones entire all territory of Cairo 500 substation with electric field below and above international exposure limits for different workers heights, 1m, 1.5m and 1.8m. ERange(kV/m) ElectricfieldbelowPublicexposurelimit (0≤Е<5) ElectricfieldbelowICNIRPoccupational exposurelimit (5≤Е<10) ElectricfieldaboveICNIRPoccupational exposurelimitorbelowIEEEoccupational exposurelimit (10≤Е<20) ElectricfieldaboveICNIRPorIEEE occupationalexposurelimit (E>20) Territory,%, For workers of height 1m 45.5% 23.81% 28.07% 2.62% Territory,%, For workers of height 1.5m 43.39% 23.99% 27.42% 5.20% Territory,%, For workers of height 1.8m 42.03% 23.57% 25.97% 8.43% Table 3. The distribution of Electric Field strength over all territory of 220 kV switchyard area for different workers heights. The part of 220 kV switchyard territory,%, where the electric field is in the range (E in kV/m) ERange (kV/m) 0≤Е<5 5≤Е<10 10≤Е<15 Territory,%, For workers of height 1m 76.7% 23.3% 0% Territory,%, For workers of height 1.5m 72.29% 25.32% 2.39% Territory,%, For workers of height 1.8m 71.56% 24.03% 4.29%
  • 10.  ISSN: 2252-8792 IJAPE Vol. 3, No. 3, December 2014 : 175 – 189 184 Table (4): The distribution of Electric Field strength over all territory of 500 kV switchyard area for different workers heights. The part of 500 kV switchyard 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,%, For workers of height 1m 24.81 32.54 14.71 21.76 6.18 0 Territory,%, For workers of height 1.5m 22.56 31.68 15.81 18.35 11.14 0.46 Territory,%, For workers of height 1.8m 20.37 30.35 16.39 15.41 15.58 1.9 According to all investigations achieved above for different workers heights during working in live condition at normal operation, the maximum values of the electric field strength obtained at most territory of this substation are less than 20 kV/m (the guidelines of the IEEE Std. C95.6 for occupational exposure) except only at certain few points (not exceeds 2.62% for workers of 1m height, 5.2% for workers of 1.5m height and 8.43% for workers of 1.8m height of overall substation territory) in this substation it reaches and exceeds 20 kV/m. These results are good matched and agreed with other related studies [11-13]. 5.2. Electric Field Distribution During Live Line Maintenance This study was conducted not only for a workers standing on the ground surface with his foot in switchyards during normal operation (hot-stick position), but also for a workers in live line maintenance position (bare hand position) under actual loading conditions. This field is calculated inside this modeled typical HV substation at a height levels of 8m, 11m, 14m and 17m above ground, approximating the height level of a workman above ground level during live line maintenance, as positions for live line working condition inside this substation nearby and underneath 220 kV busbars, 500 kV busbars, 220 kV ingoing and outgoing feeders and 500 kV ingoing and outgoing feeders respectively. This field is calculated without considering the effects of insulating/protective clothes. Figures 14-a, 14-b, 15-a, 15-b, 16-a, 16-b, 17-a and 17-b present the electric field distribution over all territory of 500 kV and 220 kV switchyards at live line maintenance height levels described previously in the form of contours map and 3D surface map respectively. From these figures, it is noticed that the maximum electric field values imposed to the human body during bare-hand position are 64.99 kV/m for height of 8m and occurs at position (x=210 m and y=90 m) located under 220 kV Bus-2, 134.02 kV/m for height of 11m and occurs at position (x=288 m and y=345 m) located under 500 kV Bus-1, 200.62 kV/m for height of 14m and occurs at position (x=60 m and y=75 m) located underneath 220 kV Buses and 214.89 kV/m for height of 17m and occurs at position (x=66 m and y=295 m) located under 500 kV Bus-1. According to all investigations achieved above for all cases and positions of workers during working in live line maintenance, the maximum values of the electric field strength obtained are good matched and consistent with other related studies [14,15].
  • 11. IJAPE ISSN: 2252-8792  Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan) 185 Figure 14. a. Contour map for the electric-field strength distribution throughout 220 kV switchyard area, at 8m above ground level. Figure 14.B. Surface map for the electric-field strength distribution throughout 220 kV switchyard area, at 8m above ground level. Figure (15-a): Contour map for the electric-field strength distribution throughout 500 kV switchyard area, at 11m above ground level. Figure (15-b): Surface map for the electric-field strength distribution throughout 500 kV switchyard area, at 11m above ground level. Figure 16.a. Contour map for the electric-field strength distribution throughout 220 kV switchyard area, at 14m above ground level. Figure 16.b. Surface map for the electric-field strength distribution throughout 220 kV switchyard area, at 14m above ground level 0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 Distance along Lateral Direction (m) 0 20 40 60 80 100 120 140 160 180 200 220 DistancealongLongitudinalDirection(m) 0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 Distance along Lateral Direction (m) 240 260 280 300 320 340 360 380 400 DistancealongLongitudinalDirection(m) 0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 Distance along Lateral Direction (m) 0 20 40 60 80 100 120 140 160 180 200 220 DistancealongLongitudinalDirection(m)
  • 12.  ISSN: 2252-8792 IJAPE Vol. 3, No. 3, December 2014 : 175 – 189 186 Figure 17.a. Contour map for the electric-field strength distribution throughout 500 kV switchyard area, at 17m above ground level. Figure (17-b): Surface map for the electric-field strength distribution throughout 500 kV switchyard area, at 17m above ground level. 6. MEASUREMENTS RESULTS AND DISCUSSIONS The electric field produced inside this typical 500/220 kV substation is measured and profiled at a longitudinal distances along 500kV and 220kV ingoing and outgoing lines, while it has been measured at a lateral distances, along 500kV and 220kV bus bars. During these measurements, the electric sensor module (HI 3604 ELF Survey Meter) should be placed far away from the human on a wooden tripod base unit, such that the human body interference on the electric field measurements is avoided, and a fiber optic cable is used to connect it to the base unit [16, 17]. The methodology of electric field measurements under buses and lines conductors was conducted at a height of 1.5m above the ground to study the field levels experienced by human beings through 301 measurement points under each phase of buses' conductors, 76 measurement points under each phase of 500 kV incoming feeders' conductors, 91 measurement points under each phase of 500 kV outgoing feeders' conductors, 161 measurement points under each phase of 220 kV incoming feeders' conductors and 71 measurement points under each phase of 220 kV outgoing feeders' conductors. Figures 18, 19, 20 and 21 show the longitudinal electric field profiles measured and calculated along 500kV and 220kV bus bars and along 500kV outgoings and 220kV ingoings respectively. These measurements showed that the electric field strength values are higher than the safe occupational exposure limits at certain positions inside this substation. Table (5) shows the maximum measured and calculated electric field strength values along all buses and feeders mentioned above. From these tables, it is observed that the simulation results are consistent with the measured values with very small tolerance 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. Table 5. Maximum measured and calculated electric field values along all buses and feeders of Cairo 500 substation at height of 1.5m Location Max. Measured Elec. Field (kV/m) Max. Calculated Elec. Field (kV/m) Error, % Along 500 kV Buses 24.7 25.6 3.6% Along 500 kV INC.s 16.68 16.23 2.7% Along 500 kV OUT.s 16.66 16.82 0.96% Along 220 kV Buses 10.56 11 4.2% Along 220 kV INC.s 10.51 10.17 3.2% Along 220 kV OUT.s 10.44 9.97 4.5% 0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 Distance along Lateral Direction (m) 240 260 280 300 320 340 360 380 400 DistancealongLongitudinalDirection(m)
  • 13. IJAPE ISSN: 2252-8792  Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan) 187 Figure 18. Longitudinal electric field profiles measured and calculated along 500kV Buses inside Cairo 500 Substation. Figure 19. Longitudinal electric field profiles measured and calculated along 220kV Buses inside Cairo 500 Substation. Figure 20. Longitudinal electric field profiles measured and calculated along 500kV OUT.s inside Cairo 500 Substation. 0 50 100 150 200 250 300 0 0.5 1 1.5 2 2.5 3 x 10 4 Distance along Bus Length X(m) TotalElectricFieldintensityE(V/m) Total Electric Field Profile along 500kV Buses- Calculated Vs Measured at height of 1.5m Cal. Field along Bus-1 (Y=350) Meas. Field along Bus-1 (Y=350) Cal. Field along Bus-2 (Y=300) Meas. Field along Bus-2 (Y=300) 0 50 100 150 200 250 300 0 2000 4000 6000 8000 10000 12000 Distance along Bus Length X(m) TotalElectricFieldintensityE(V/m) Total Electric Field Profile along 220kV Buses- Calculated Vs Measured at height of 1.5m Cal. Field along Bus-1 (Y=50) Meas. Field along Bus-1 (Y=50) Cal. Field along Bus-2 (Y=90) Meas. Field along Bus-2 (Y=90) 230 240 250 260 270 280 290 300 310 320 330 0 2000 4000 6000 8000 10000 12000 14000 16000 18000 Distance along outgoing Length Y(m) TotalElectricFieldintensityE(V/m) Total Electric Field Profile along 500kV out Feeders- Calculated Vs Measured at height of 1.5m Cal. Field along outgoing-1 (X=75) Meas. Field along outgoing-1 (X=75) Cal. Field along outgoing-2 (X=150) Meas. Field along outgoing-2 (X=150) Cal. Field along outgoing-3 (X=225) Meas. Field along outgoing-3 (X=225)
  • 14.  ISSN: 2252-8792 IJAPE Vol. 3, No. 3, December 2014 : 175 – 189 188 Figure 21 Longitudinal electric field profiles measured and calculated along 220kV INC.s inside Cairo 500 Substation. 7. CONCLUSIONS AND RECOMMENDATIONS In this study, a method is proposed for investigation the distribution of the electric field produced inside HV substations. This method is based on the charge simulation technique and the most important results from this study are as follows:  During working in live condition at normal operation inside 500/220 kV substations (hot- stick position), the maximum values of the electric field strength at most territory of this substation are less than 20 kV/m (the guidelines of the IEEE Std. C95.6 for occupational exposure) except only at certain few points (not exceeds 2.62% for workers of 1m height, 5.2% for workers of 1.5m height and 8.43% for workers of 1.8m height of overall substation territory) it exceeds 20 kV/m.  By increasing the workers/calculation height, the density of electric fields nearby and underneath busbars, ingoing and outgoing feeders increased and the area of zone of security (E<5 kV/m) entire territory of modelled substation decreased while the area of zone of influence (E>5 kV/m) increased.  During working in live condition as live line maintenance inside 500/220 kV substations (Bar-hand position), the values of the electric field strength are more danger while its maximum values exceed 25 kV/m with about 8.6 times, where the presence without personal protective equipment is much prohibited.  All simulation results are good matched and consistent with measurements results and other related studies.  It is recommended for using this study for planning service works or for inspection of equipment inside high voltage power transformation substations. 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, Vol. 238. Geneva, 2007. [3] IEEE Std. Safety Levels With Respect to Human Exposure to Electromagnetic Fields, 0 to 3 kHz, IEEE Std. C95.6-2002, Oct. 2002. [4] International Commission on Non-Ionizing Radiation Protection (ICNIRP), Guidelines for limiting exposure to time-varying electric and magnetic fields (1 Hz to 100 kHz), Vol. 99, No. 6, 818-836 Health Physics, 2010. [5] National Radiological Protection Board (NRPB), Advice on limiting exposure to electromagnetic fields (0-300 GHz), Vol. 15, No. 2, 2004. [6] "Directive 2004/40/EC of the European Parliament and of the Council of 29th April 2004 on “the minimum health and safety requirements regarding the exposure of workers to the risk arising from physical agents (electromagnetic fields)” (18th individual Directive within the meaning of Article 16(1) of Directive 89/391/EEC)‟, Official Journal . [7] H. Singer, H. Steinbigler, P. Weiss, "A Charge Simulation Method for the Calculation of High Voltage Fields", IEEE Trans. on PAS, Vol. 93, P-P: 1660-1667, 1974. [8] E.kuffel, W.S. Zaengle and J. Kuffel, “High Voltage Engineering, Fundamentals”, Second edition reprint, 2001 (Text book). 60 80 100 120 140 160 180 200 220 240 0 2000 4000 6000 8000 10000 12000 Distance along Incoming Length Y(m) TotalElectricFieldintensityE(V/m) Total Electric Field Profile along 220kV INC Feeders- Calculated Vs Measured at height of 1.5m Cal. Field along Incoming-1 (X=56.25) Meas. Field along Incoming-1 (X=56.25) Cal. Field along Incoming-2 (X=150) Meas. Field along Incoming-2 (X=150) Cal. Field along Incoming-3 (X=243.75) Meas. Field along Incoming-3 (X=243.75)
  • 15. IJAPE ISSN: 2252-8792  Investigation of Electric Field Distribution Inside 500/220 kV Transformation… (Essam M. Shaalan) 189 [9] Nazar H. Malik, “A review of the Charge Simulation Method and its Applications” IEEE Transactions on Electrical Insulation, Vol. 24, No. 1, P-P: 3–20, February 1989. [10] 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. [11] I.S. Okrainskaya, S.P. Gladyshev, A.I. SidorovAnd N.V. Glotova, “Investigation of Electric Field Distribution Inside 500 kV Power Distribution Substations”, IEEE International Conference on Electro/ Information Technology (EIT), P-P: 1 – 4, Rapid City, SD, 9-11 May 2013. [12] I. S. Okrainskaya, A. V. Babin, A. I. Sidorov, et al., “General Characteristic of Electric Field Intensity of 500 kV Outdoor Switchgears”, Power Technology and Engineering, Vol. 40, No. 2, P-P: 45 – 48, 2006. Translated from Élektricheskie Stantsii, No. 1, January 2006. [13] A.S. Safigianni, A.I. Spyridopoulos and V.L. Kanas, “Electric and Magnetic Field Measurements in a High Voltage Center”, Ann. British Occupational Hygiene Society, Vol. 56, No. 1, P-P: 18–24, 2012. [14] Samy M. Ghania, “Evaluation of Electromagnetic Fields Exposure during Live Line Working Conditions Inside High Voltage Substations”, IRACST - Engineering Science and Technology: An International Journal (ESTIJ), ISSN: 2250-3498, Vol. 3, No. 1, P-P: 199 – 206, February 2013. [15] 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. [16] HI 3604 ELF Survey Meter User‟s Manual, Holladay Ind. 2002. [17] HI-4413 Fiber Optic RS-232 Interface With Probe View™ 3600 User‟s manual, 2002 BIOGRAPHIES OF AUTHORS Sayed Abo-Elsood S. Ward: 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, faculty of engineering (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 Mohamed A. Ghania: Ghania was born in Egypt on December 28, 1971. He received the B.Sc., M.Sc., and Ph.D. degrees in electrical engineering from Faculty of Engineering (Shoubra), 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 modeling and simulation of electrical machines, drives for electrical vehicles, studying the human exposure to high voltage electromagnetic fields. Essam Mohamed A. Shaalan: 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, Faculty of Engineering (Shoubra), Cairo, Egypt. He received the M.Sc. degrees in electrical engineering from Benha University, Faculty of Engineering (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 studying the effect of these fields on human/workers.