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TELKOMNIKA, Vol.17, No.4, August 2019, pp.2001~2007
ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018
DOI: 10.12928/TELKOMNIKA.v17i4.12765  2001
Received December 13, 2018; Revised March 8, 2019; Accepted April 10, 2019
Space charges analysis on insulator
with uniform layer contamination effect
Mohd Haris Asyraf Shee Kandar
1
, Nor Akmal Mohd Jamail*
2
, Qamarul Ezani Kamarudin
3
,
Nordiana Azlin Othman
4
, Nor Asiah Muhamad
5
1,2,4
Faculty of Electrical and Electronic Engineering, Universiti Tun Hussein Onn Malaysia (UTHM),
86400 Batu Pahat, Johor, Malaysia
3
Faculty of Mechanical and Manufacturing Engineering, Universiti Tun Hussein Onn Malaysia (UTHM),
86400 Batu Pahat, Johor, Malaysia
5
School of Electrical and Electronic Engineering, Universiti Sains Malaysia, Malaysia
*Corresponding author, e-mail: haris_asyraf@ymail.com
1
, norakmal@uthm.edu.my
2
,
ezani@uthm.edu.my
3
, ndiana@uthm.edu.my
4
, norasiah.m@usm.my
5
Abstract
High voltage direct current (HVDC) transmission provides an attractive alternative for bulk power
transfer. However, HVDC transmission may have loss about half per unit length of high voltage alternating
current (HVAC) at the same amount of power carried. This is due to the space charge formation around
the conductor in HVDC cables. It is known that the presence of space charge inside an insulator may
distort the local electric field and surface energy. This paper investigates the effect of electrostatics for
space charge, electric field and surface energy in the HVDC cable in clean and contaminated conditions.
The effect of uniform layer contamination from oil, sandstone and fresh water was conducted on 11 kV
XLPE cable using finite element software under electrostatics study. The contamination layer was created
around the XLPE cable by multifarious the radius of layer contamination from the conductor.
The simulation results show that enlargement of contamination layer radius by 1.0 mm (light), 1.5 mm
(medium) and 2.0 mm (heavy) resulted in the reduction of surface energy by 20% and electric field by 22%
but increase the space charge amplitude by 76%. The study also found that fresh water can be considered
as the worst contamination compared to oil and sandstone.
Keywords: contamination, electric field, space charge, surface energy, XLPE
Copyright © 2019 Universitas Ahmad Dahlan. All rights reserved.
1. Introduction
Technology in HVDC transmission has managed many industrialists in the world to
invest polymer in direct current (DC) on power cables. Polymeric insulation such XLPE is
the most commonly used and best insulator in features [1-8], when used with DC operation may
inconsistently lead to a problem. Space charge inside the insulated material increased due to
the lowest carrier mobility and high trapped rate in certain states, increased the space charge
through the body of the insulated material.
Understanding the concept of space charge is the most importance because the space
charge accumulates on interfaces. Permittivity and conductivity also not same on the different
layers [9] and an electric charge is treated over a region of space [10]. Through this concept,
space charge can be determined by the thickness of insulator and various types of uniform layer
contamination. While the voltage and electric field distribution can be calculated by finite
element software.
Researcher [11] had explained molecular structure and chemically bonded of
cross-linked polyethylene where it easy deform at extraordinary temperature. While linear
molecular structure and chemical bonded strongly resist to deform even at extraordinary
temperature.According to the parameter of HVDC cable, every model of HVDC can be designed
by using Quickfield software and simulation have been shown the results of space charge,
electric field and surface energy for various types of uniform later contamination. Various types
of uniform layer contamination have been displayed different effect on space charge.
Cross-Linked Polyethylene (XLPE)
XLPE materials are derived through processes which cause a cross-bonding [12].
Polyethylene has a linear molecular structure as shown in Figure 1 (a) molecules of
polyethylene not chemically bonded as shown in Figure 1 (b) are easily deformed at high
 ISSN: 1693-6930
TELKOMNIKA Vol. 17, No. 4, August 2019: 2001-2007
2002
temperature, while XLPE molecules bonded in a three dimensional network as shown in
Figures 2 (a) and 2 (b) have strong resistance to deformation even at high temperature [11, 13].
(a) (b) (a) (b)
Figure 1. Molecular structure and chemically
bonded of polyethylene (a) molecular structure
of polyethylene (molecular structure)
(b) chemically bonded of polyethylene
molecules (chemically bonded) [11, 13]
Figure 2. Linear molecular structure and
chemically bonded of polyethylene
(a) structure of polyethylene (linear
molecular structure) (b) polyethylene
molecules (chemically bonded) [11, 13]
Cross-linked polyethylene is produced from polyethylene under high pressure with
organic peroxides as additives. The application of heat and pressure is used to effect the cross
linking. This causes the individual molecular chains to link with one another which in turn causes
the material to change from a thermoplastic to an elastic material [11].
An important advantage of XLPE as insulation for medium and high voltage cables is
their low dielectric loss. The dielectric loss factor is about one decimal power lower than that of
paper insulated cables and about two decimal powers lower than that of Polyvinyl Chloride
(PVC) insulated cables. Since the dielectric constant is also more favorable, the mutual
capacitance of XLPE cables is also lower, thus reduced the charged currents and earth-leakage
currents in networks without the rigid star point earthed [11].
2. Research Method
This part explained about research method to gain simulation results of space charge,
surface energy and electric field of XLPE insulator by using Quickfield Software.
2.1. Space Charge Measurement Setting
Gauss’s law states that the net electric flux through any closed surface is equal to the
total charge enclosed by that surface. In a like manner, total electric charge, Q in particular
volume can be calculated as a flux of electric displacement, D over its closed boundary and
written as [14]:
( . )
s
Q D n dS 
(1)
2.2. Electric Field Measurement Setting
High voltage cable almost always have a coaxial configuration with conductor of inner
and outer radius of a and b, respectively. When a test voltage, is applied across the cable,
a charge q = C is produced on the cable’s conductor where , and C are relative
permitivitty, space permitivitty and capacitance value of the insulation. By application Gauss’s
Law, the electric stress, E in the coaxial cable insulation at a distance r from the cable center is
given as [15]:
02
T T
r
r
CV V
E
br
r In
a
   
 




(2)
2.3. Surface Energy Measurement Setting
Electrostatic potential energy is a measure of the energy stored in the electric field
where , E and D are surface energy, electric field strength and electric displacement and is
given by [14]:
TELKOMNIKA ISSN: 1693-6930 
Space charges analysis on insulator with uniform layer... (Mohd Haris Asyraf Shee Kandar)
2003
½ ( . )s
s
W E D dS  (3)
2.4. Material Properties
The material properties and contamination layer thickness used in this simulation study
is shown in Table 1 and Table 2, respectively.
Table 1. Materials Properties Used
for Simulation Purpose [13, 16-23]
Material Relative Permittivity,
XLPE 2.30
Oil 2.00 - 2.40
Sandstone 4.65
Fresh water at 75 ᵒF 78.30
Table 2. Contamination
Layers Thickness [24]
Contamination Level Thickness
Light 1.0mm
Medium 1.5mm
Heavy 2.0mm
Clean None
2.5. Design Model and Simulation Parameter
The insulator of XLPE cable was modelled and designed by using QuickField software.
Cable model and parameter are shown in Figure 3. Figures 4 and 5 illustrate cable model after
mesh setting for with and without contamination in 2D and 3D views. In this paper, the problem
type of electrostatics has been chosen to analyse the space charge, electric fields and surface
energy of the XLPE insulation. For parameter setting, the coordinate system is in Cartesian, the
length of cable is 1000mm and the length units are in millimetre (mm). Plane parallel (model
class) was chosen because length is on the z-axis.
Figure 3. HVDC cable profile and dimensions
(a) (b) (a) (b)
Figure 4. 3D views (a) Normal HVDC cable
without contamination (b) HVDC cable with
contamination
Figure 5. 2D views (a) Normal HVDC
cable without contamination (b) HVDC
cable with contamination
3. Results and Analysis
In this section, it is explained the simulation results of space charge, electric field and
surface energy of XLPE insulator by using Quickfield Software.
3.1. Simulation Results for Space Charge, Surface Energy and Electric Field on XLPE
Insulation
The simulation and analysis results for the XLPE insulation is to find the space charge,
surface energy and electric field strength in XLPE insulation without oil, sandstone and fresh
water contamination. The space charge and the electric field result can be viewed from
 ISSN: 1693-6930
TELKOMNIKA Vol. 17, No. 4, August 2019: 2001-2007
2004
the colour map shown in Figure 6 (a) and Figure 6 (b). It is apparent that red colour map
because the highest and lowest value of space charge depends on cross sectional area. The
value for space charge is 264.55nC. Nevertheless, electric field can be viewed from the colour
map and the value referred to the legend. The diagram shows the value of the electric field fall
off from the conductor to ground. For electric field, legend shown that red colour indicates as
greater voltage while blue colour indicates as ground. The value for surface energy is 14.61J/m
as shown in Figure 6(c) and cross sectional area influence highest and lowest value.
However, the contamination layer for space charge is bigger than without contamination
layers which is 2362.00 nC compared to 2098.30 nC shown in Figure 7 (a). Prior to this,
contamination layers contain more cross sectional area compared to the area without
contamination layers. While the value for the electric field on contamination layer is zero based on
the colour map in Figure 7 (b) because in ground mode.This factor contribute to surface energy
where it is lower than without contamination layers which is 5.91J/m compared to 8.67 J/m in
Figure 7 (c). Similarly, same concept for space charge was applied to surface energy.
(a) (a)
(b) (b)
(c) (c)
Figure 6. Colour map and integral calculator
for HVDC cable without contamination
(a) space charge (b) electric field
(c) surface energy
Figure 7. Colour map and integral calculator
for HVDC cable with contamination (a) space
charge (b) electric field (c) surface energy
Another essential point, the electric field strength for HVDC insulation cable without oil,
sandstone and fresh water contamination are shown in Figure 8 (a). Based on the graph, the
electric field declined from 0.0mm to 3.4 mm which start around the conductor until the ground.
The electric field strength is enhancing at 4078220 V/m when close around the conductor and
become weaker at 0V/m when near to ground. In comparison, Figure 8 (b) shows HVDC cable
with oil contamination for electric field strength. The electric field also decayed from 0.0mm to
TELKOMNIKA ISSN: 1693-6930 
Space charges analysis on insulator with uniform layer... (Mohd Haris Asyraf Shee Kandar)
2005
3.4 mm which is started from the conductor to the ground of the cable. Electric field strength is
mark up at 4064460V/m around the conductor and become lessen at 0 V/m when near to
ground. It has been shown that the electric field at the contamination layer is 0 V/m that starts
from 3.4 mm to 4.4 mm.
(a) (b)
Figure 8. Electric field strength (a) without contamination (b) with contamination
3.2. Simulation Results for Space Charge, Surface Energy and Electric Field on XLPE
Insulation with Different Contamination Level and Source
Table 3 compares the simulation results of space charge in clean and contaminated
conditions. The result shows that fresh water contamination has higher space charge compared
to oil and sandstone in all conditions. As might be expected that high permittivity of fresh water
produce much more space charge in the insulator [25].
Figure 9 shows the distribution of space charge in clean conditions is quite similar for all
contamination sources; where the huge difference at heavy between fresh water and sandstone
which approximately 49 percent. For contaminated conditions, there is a clear trend of the
space charge distribution increases as the contamination levels is increase. J.W. (1998)
disputed [25] that the presences of contamination can effect an uncontrolled increase in the
generation rates of free charge.
Table 3. Space Charge and Surface Energy in Clean and Contaminated Conditions
Condition of HVDC cable
Space Charge,
(nC)
Surface Energy,
(
Electric Field, (
Simulation
Contamination
Level
Contamination
Source
Simulation
Minimum Maximum
Clean
Normal (Without
Contamination)
264.55 14.61
0
4.27
Light
Oil
Sandstone
Fresh Water
263.70
497.40
497.40
14.58
13.75
13.75
4.18
4.00
4.00
Medium
Oil
Sandstone
Fresh Water
320.40
529.10
1015.00
14.43
13.64
12.43
4.14
3.88
3.64
Heavy
Oil
Sandstone
Fresh Water
497.40
564.20
1113.70
13.76
13.00
11.75
4.00
3.76
3.35
(a) (b) (c)
Figure 9. Space charge distribution for (a) oil contamination, (b) sandstone contamination,
and (c) fresh water contamination
 ISSN: 1693-6930
TELKOMNIKA Vol. 17, No. 4, August 2019: 2001-2007
2006
Table 3 and Figure 10 demonstrate the simulation of surface energy in clean and
contaminated conditions for all contamination sources. Complementary to this it is analyzed
from the tabulated results that the surface energy for fresh water at the heavy condition of
HVDC cable insulation for simulation result is wither than the surface energy at normal HVDC
cable insulation which is 11.75 J/m compared to 14.61 J/m. The surface energy at fresh water
contamination is lower than the surface energy at the oil and sandstone contamination due to
high permittivity of contaminant. Due to contaminant molecules change the balance of forces
and reduce the net inward force. Since the net inward force is related to the surface energy, the
surface energy is reduced by contaminant and was investigated in [26]. Thus, it can cause
damage and poor performance of the cable.
When Gauss’s law is applied, minimum electric field is zero as shown in Table 3 and
Figure 11. Equally important, apply the Gauss’s law and there is no charge inside that insulator
that the electric field will be zero, so outside zero and here in the core also zero. Maximum electric
field for normal at clean HVDC cable insulation for simulation result is 4.27x10 V/m strengthens
than the electric field for fresh water at the heavy condition of HVDC cable insulation which is
3.35x10 V/m. In short, high permittivity of fresh water also shows the weaken electric field at
contamination compared to the electric field at oil and sandstone contamination. Similarly,
Malik et al. [15] stated that electric field is inversely proportional to the permittivity.
(a) (b) (c)
Figure 10. Surface energy for (a) oil contamination, (b) sandstone contamination,
and (c) fresh water contamination
(a) (b) (c)
Figure 11. Electric field for (a) oil contamination, (b) sandstone contamination,
and (c) fresh water contamination
4. Conclusion
In a nutshell, by using this software, XLPE cable with the effect of uniform layer
contamination of oil, sandstone and fresh water have been analysed by multifarious the
condition level and source of contamination. It was shown that the space charge became higher
when the radius of contamination is greater while electric field and surface energy are depressed.
In brief, fresh water can be justified as the worst among oil and sandstone due to high
permittivity. To sum up, normal HVDC insulation cable without contamination can be highlighted
as superior through performances and capabilities where it produce inferior space charge.
Acknowledgement
The authors gratefully acknowledge the Research Management Centre of Universiti Tun
Hussein Onn Malaysia under grant GPPS vote U953, Research Fund, UTHM, Kvolt Focus
Group Team, and High Voltage Laboratory UTHM for the equipment support.
TELKOMNIKA ISSN: 1693-6930 
Space charges analysis on insulator with uniform layer... (Mohd Haris Asyraf Shee Kandar)
2007
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Space charges analysis on insulator with uniform layer contamination effect

  • 1. TELKOMNIKA, Vol.17, No.4, August 2019, pp.2001~2007 ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018 DOI: 10.12928/TELKOMNIKA.v17i4.12765  2001 Received December 13, 2018; Revised March 8, 2019; Accepted April 10, 2019 Space charges analysis on insulator with uniform layer contamination effect Mohd Haris Asyraf Shee Kandar 1 , Nor Akmal Mohd Jamail* 2 , Qamarul Ezani Kamarudin 3 , Nordiana Azlin Othman 4 , Nor Asiah Muhamad 5 1,2,4 Faculty of Electrical and Electronic Engineering, Universiti Tun Hussein Onn Malaysia (UTHM), 86400 Batu Pahat, Johor, Malaysia 3 Faculty of Mechanical and Manufacturing Engineering, Universiti Tun Hussein Onn Malaysia (UTHM), 86400 Batu Pahat, Johor, Malaysia 5 School of Electrical and Electronic Engineering, Universiti Sains Malaysia, Malaysia *Corresponding author, e-mail: haris_asyraf@ymail.com 1 , norakmal@uthm.edu.my 2 , ezani@uthm.edu.my 3 , ndiana@uthm.edu.my 4 , norasiah.m@usm.my 5 Abstract High voltage direct current (HVDC) transmission provides an attractive alternative for bulk power transfer. However, HVDC transmission may have loss about half per unit length of high voltage alternating current (HVAC) at the same amount of power carried. This is due to the space charge formation around the conductor in HVDC cables. It is known that the presence of space charge inside an insulator may distort the local electric field and surface energy. This paper investigates the effect of electrostatics for space charge, electric field and surface energy in the HVDC cable in clean and contaminated conditions. The effect of uniform layer contamination from oil, sandstone and fresh water was conducted on 11 kV XLPE cable using finite element software under electrostatics study. The contamination layer was created around the XLPE cable by multifarious the radius of layer contamination from the conductor. The simulation results show that enlargement of contamination layer radius by 1.0 mm (light), 1.5 mm (medium) and 2.0 mm (heavy) resulted in the reduction of surface energy by 20% and electric field by 22% but increase the space charge amplitude by 76%. The study also found that fresh water can be considered as the worst contamination compared to oil and sandstone. Keywords: contamination, electric field, space charge, surface energy, XLPE Copyright © 2019 Universitas Ahmad Dahlan. All rights reserved. 1. Introduction Technology in HVDC transmission has managed many industrialists in the world to invest polymer in direct current (DC) on power cables. Polymeric insulation such XLPE is the most commonly used and best insulator in features [1-8], when used with DC operation may inconsistently lead to a problem. Space charge inside the insulated material increased due to the lowest carrier mobility and high trapped rate in certain states, increased the space charge through the body of the insulated material. Understanding the concept of space charge is the most importance because the space charge accumulates on interfaces. Permittivity and conductivity also not same on the different layers [9] and an electric charge is treated over a region of space [10]. Through this concept, space charge can be determined by the thickness of insulator and various types of uniform layer contamination. While the voltage and electric field distribution can be calculated by finite element software. Researcher [11] had explained molecular structure and chemically bonded of cross-linked polyethylene where it easy deform at extraordinary temperature. While linear molecular structure and chemical bonded strongly resist to deform even at extraordinary temperature.According to the parameter of HVDC cable, every model of HVDC can be designed by using Quickfield software and simulation have been shown the results of space charge, electric field and surface energy for various types of uniform later contamination. Various types of uniform layer contamination have been displayed different effect on space charge. Cross-Linked Polyethylene (XLPE) XLPE materials are derived through processes which cause a cross-bonding [12]. Polyethylene has a linear molecular structure as shown in Figure 1 (a) molecules of polyethylene not chemically bonded as shown in Figure 1 (b) are easily deformed at high
  • 2.  ISSN: 1693-6930 TELKOMNIKA Vol. 17, No. 4, August 2019: 2001-2007 2002 temperature, while XLPE molecules bonded in a three dimensional network as shown in Figures 2 (a) and 2 (b) have strong resistance to deformation even at high temperature [11, 13]. (a) (b) (a) (b) Figure 1. Molecular structure and chemically bonded of polyethylene (a) molecular structure of polyethylene (molecular structure) (b) chemically bonded of polyethylene molecules (chemically bonded) [11, 13] Figure 2. Linear molecular structure and chemically bonded of polyethylene (a) structure of polyethylene (linear molecular structure) (b) polyethylene molecules (chemically bonded) [11, 13] Cross-linked polyethylene is produced from polyethylene under high pressure with organic peroxides as additives. The application of heat and pressure is used to effect the cross linking. This causes the individual molecular chains to link with one another which in turn causes the material to change from a thermoplastic to an elastic material [11]. An important advantage of XLPE as insulation for medium and high voltage cables is their low dielectric loss. The dielectric loss factor is about one decimal power lower than that of paper insulated cables and about two decimal powers lower than that of Polyvinyl Chloride (PVC) insulated cables. Since the dielectric constant is also more favorable, the mutual capacitance of XLPE cables is also lower, thus reduced the charged currents and earth-leakage currents in networks without the rigid star point earthed [11]. 2. Research Method This part explained about research method to gain simulation results of space charge, surface energy and electric field of XLPE insulator by using Quickfield Software. 2.1. Space Charge Measurement Setting Gauss’s law states that the net electric flux through any closed surface is equal to the total charge enclosed by that surface. In a like manner, total electric charge, Q in particular volume can be calculated as a flux of electric displacement, D over its closed boundary and written as [14]: ( . ) s Q D n dS  (1) 2.2. Electric Field Measurement Setting High voltage cable almost always have a coaxial configuration with conductor of inner and outer radius of a and b, respectively. When a test voltage, is applied across the cable, a charge q = C is produced on the cable’s conductor where , and C are relative permitivitty, space permitivitty and capacitance value of the insulation. By application Gauss’s Law, the electric stress, E in the coaxial cable insulation at a distance r from the cable center is given as [15]: 02 T T r r CV V E br r In a           (2) 2.3. Surface Energy Measurement Setting Electrostatic potential energy is a measure of the energy stored in the electric field where , E and D are surface energy, electric field strength and electric displacement and is given by [14]:
  • 3. TELKOMNIKA ISSN: 1693-6930  Space charges analysis on insulator with uniform layer... (Mohd Haris Asyraf Shee Kandar) 2003 ½ ( . )s s W E D dS  (3) 2.4. Material Properties The material properties and contamination layer thickness used in this simulation study is shown in Table 1 and Table 2, respectively. Table 1. Materials Properties Used for Simulation Purpose [13, 16-23] Material Relative Permittivity, XLPE 2.30 Oil 2.00 - 2.40 Sandstone 4.65 Fresh water at 75 ᵒF 78.30 Table 2. Contamination Layers Thickness [24] Contamination Level Thickness Light 1.0mm Medium 1.5mm Heavy 2.0mm Clean None 2.5. Design Model and Simulation Parameter The insulator of XLPE cable was modelled and designed by using QuickField software. Cable model and parameter are shown in Figure 3. Figures 4 and 5 illustrate cable model after mesh setting for with and without contamination in 2D and 3D views. In this paper, the problem type of electrostatics has been chosen to analyse the space charge, electric fields and surface energy of the XLPE insulation. For parameter setting, the coordinate system is in Cartesian, the length of cable is 1000mm and the length units are in millimetre (mm). Plane parallel (model class) was chosen because length is on the z-axis. Figure 3. HVDC cable profile and dimensions (a) (b) (a) (b) Figure 4. 3D views (a) Normal HVDC cable without contamination (b) HVDC cable with contamination Figure 5. 2D views (a) Normal HVDC cable without contamination (b) HVDC cable with contamination 3. Results and Analysis In this section, it is explained the simulation results of space charge, electric field and surface energy of XLPE insulator by using Quickfield Software. 3.1. Simulation Results for Space Charge, Surface Energy and Electric Field on XLPE Insulation The simulation and analysis results for the XLPE insulation is to find the space charge, surface energy and electric field strength in XLPE insulation without oil, sandstone and fresh water contamination. The space charge and the electric field result can be viewed from
  • 4.  ISSN: 1693-6930 TELKOMNIKA Vol. 17, No. 4, August 2019: 2001-2007 2004 the colour map shown in Figure 6 (a) and Figure 6 (b). It is apparent that red colour map because the highest and lowest value of space charge depends on cross sectional area. The value for space charge is 264.55nC. Nevertheless, electric field can be viewed from the colour map and the value referred to the legend. The diagram shows the value of the electric field fall off from the conductor to ground. For electric field, legend shown that red colour indicates as greater voltage while blue colour indicates as ground. The value for surface energy is 14.61J/m as shown in Figure 6(c) and cross sectional area influence highest and lowest value. However, the contamination layer for space charge is bigger than without contamination layers which is 2362.00 nC compared to 2098.30 nC shown in Figure 7 (a). Prior to this, contamination layers contain more cross sectional area compared to the area without contamination layers. While the value for the electric field on contamination layer is zero based on the colour map in Figure 7 (b) because in ground mode.This factor contribute to surface energy where it is lower than without contamination layers which is 5.91J/m compared to 8.67 J/m in Figure 7 (c). Similarly, same concept for space charge was applied to surface energy. (a) (a) (b) (b) (c) (c) Figure 6. Colour map and integral calculator for HVDC cable without contamination (a) space charge (b) electric field (c) surface energy Figure 7. Colour map and integral calculator for HVDC cable with contamination (a) space charge (b) electric field (c) surface energy Another essential point, the electric field strength for HVDC insulation cable without oil, sandstone and fresh water contamination are shown in Figure 8 (a). Based on the graph, the electric field declined from 0.0mm to 3.4 mm which start around the conductor until the ground. The electric field strength is enhancing at 4078220 V/m when close around the conductor and become weaker at 0V/m when near to ground. In comparison, Figure 8 (b) shows HVDC cable with oil contamination for electric field strength. The electric field also decayed from 0.0mm to
  • 5. TELKOMNIKA ISSN: 1693-6930  Space charges analysis on insulator with uniform layer... (Mohd Haris Asyraf Shee Kandar) 2005 3.4 mm which is started from the conductor to the ground of the cable. Electric field strength is mark up at 4064460V/m around the conductor and become lessen at 0 V/m when near to ground. It has been shown that the electric field at the contamination layer is 0 V/m that starts from 3.4 mm to 4.4 mm. (a) (b) Figure 8. Electric field strength (a) without contamination (b) with contamination 3.2. Simulation Results for Space Charge, Surface Energy and Electric Field on XLPE Insulation with Different Contamination Level and Source Table 3 compares the simulation results of space charge in clean and contaminated conditions. The result shows that fresh water contamination has higher space charge compared to oil and sandstone in all conditions. As might be expected that high permittivity of fresh water produce much more space charge in the insulator [25]. Figure 9 shows the distribution of space charge in clean conditions is quite similar for all contamination sources; where the huge difference at heavy between fresh water and sandstone which approximately 49 percent. For contaminated conditions, there is a clear trend of the space charge distribution increases as the contamination levels is increase. J.W. (1998) disputed [25] that the presences of contamination can effect an uncontrolled increase in the generation rates of free charge. Table 3. Space Charge and Surface Energy in Clean and Contaminated Conditions Condition of HVDC cable Space Charge, (nC) Surface Energy, ( Electric Field, ( Simulation Contamination Level Contamination Source Simulation Minimum Maximum Clean Normal (Without Contamination) 264.55 14.61 0 4.27 Light Oil Sandstone Fresh Water 263.70 497.40 497.40 14.58 13.75 13.75 4.18 4.00 4.00 Medium Oil Sandstone Fresh Water 320.40 529.10 1015.00 14.43 13.64 12.43 4.14 3.88 3.64 Heavy Oil Sandstone Fresh Water 497.40 564.20 1113.70 13.76 13.00 11.75 4.00 3.76 3.35 (a) (b) (c) Figure 9. Space charge distribution for (a) oil contamination, (b) sandstone contamination, and (c) fresh water contamination
  • 6.  ISSN: 1693-6930 TELKOMNIKA Vol. 17, No. 4, August 2019: 2001-2007 2006 Table 3 and Figure 10 demonstrate the simulation of surface energy in clean and contaminated conditions for all contamination sources. Complementary to this it is analyzed from the tabulated results that the surface energy for fresh water at the heavy condition of HVDC cable insulation for simulation result is wither than the surface energy at normal HVDC cable insulation which is 11.75 J/m compared to 14.61 J/m. The surface energy at fresh water contamination is lower than the surface energy at the oil and sandstone contamination due to high permittivity of contaminant. Due to contaminant molecules change the balance of forces and reduce the net inward force. Since the net inward force is related to the surface energy, the surface energy is reduced by contaminant and was investigated in [26]. Thus, it can cause damage and poor performance of the cable. When Gauss’s law is applied, minimum electric field is zero as shown in Table 3 and Figure 11. Equally important, apply the Gauss’s law and there is no charge inside that insulator that the electric field will be zero, so outside zero and here in the core also zero. Maximum electric field for normal at clean HVDC cable insulation for simulation result is 4.27x10 V/m strengthens than the electric field for fresh water at the heavy condition of HVDC cable insulation which is 3.35x10 V/m. In short, high permittivity of fresh water also shows the weaken electric field at contamination compared to the electric field at oil and sandstone contamination. Similarly, Malik et al. [15] stated that electric field is inversely proportional to the permittivity. (a) (b) (c) Figure 10. Surface energy for (a) oil contamination, (b) sandstone contamination, and (c) fresh water contamination (a) (b) (c) Figure 11. Electric field for (a) oil contamination, (b) sandstone contamination, and (c) fresh water contamination 4. Conclusion In a nutshell, by using this software, XLPE cable with the effect of uniform layer contamination of oil, sandstone and fresh water have been analysed by multifarious the condition level and source of contamination. It was shown that the space charge became higher when the radius of contamination is greater while electric field and surface energy are depressed. In brief, fresh water can be justified as the worst among oil and sandstone due to high permittivity. To sum up, normal HVDC insulation cable without contamination can be highlighted as superior through performances and capabilities where it produce inferior space charge. Acknowledgement The authors gratefully acknowledge the Research Management Centre of Universiti Tun Hussein Onn Malaysia under grant GPPS vote U953, Research Fund, UTHM, Kvolt Focus Group Team, and High Voltage Laboratory UTHM for the equipment support.
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