The Correlation between Surface Tracking and Partial Discharge Characteristics on Pressboard Surface Immersed in MIDEL eN

International Journal of Electrical and Computer Engineering (IJECE)
Vol. 7, No. 2, April 2017, pp. 631~640
ISSN: 2088-8708, DOI: 10.11591/ijece.v7i2.pp631-640  631
Journal homepage: http://iaesjournal.com/online/index.php/IJECE
The Correlation between Surface Tracking and Partial
Discharge Characteristics on Pressboard Surface Immersed in
MIDEL eN
Nur Amirah Othman, Hidayat Zainuddin, Aminuddin Aman, Sharin Abd Ghani, Imran Sutan
Chairul
Research Laboratory of High Voltage Engineering, Centre for Robotics and Industrial Automation (CeRIA), Faculty of
Electrical Engineering, UniversitiTeknikal Malaysia Melaka, Hang Tuah Jaya, 76100 Durian Tunggal, Melaka, Malaysia
Article Info ABSTRACT
Article history:
Received Jun 15, 2016
Revised Feb 7, 2017
Accepted Feb 21, 2017
This paper presents the investigation of the surface tracking on pressboard
surface immersed in MIDEL eN oil. In this work, the development of surface
discharge was analyzed by correlating the visual records of surface tracking
on impregnated pressboard and the partial discharge (PD) activities. The PD
activities during the surface tracking process were analyzed in terms of Phase
Resolved Partial Discharge (PRPD) patterns. Throughout the experiment,
surface discharge is found as the development of tree-like patterns in the
form of white marks occurring on the oil-pressboard interface. This
phenomenon is generally accepted as the drying out process that involves
evaporation and decomposition of the oil molecules in the pressboard pores
due to the surface discharge activities on the pressboard surface layer. The
development of surface discharge on the pressboard surface can continue
from minutes to months or even years until failure. Thus, condition
monitoring system is important to characterize this type of faulty condition.
The experimental results show that there is the decreasing trend of PD
magnitude during the development of white mark hallway of a gap distance
which is eventually suffered from an unexpected fault.
Keyword:
Full discharge
Oil-pressboard interface
Partial discharge
Surface discharge
Transformer
Copyright © 2017 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Nur Amirah Othman,
Research Laboratory of High Voltage Engineering,
Centre for Robotics and Industrial Automation (CeRIA),
Faculty of Electrical Engineering,
Universiti Teknikal Malaysia Melaka,
Hang Tuah Jaya, 76100 Durian Tunggal, Melaka, Malaysia
Email: mira_191@yahoo.com
1. INTRODUCTION
In the past few years, manufacturers of transformer have been looking for ways to reduce the size of
transformers to decrease the manufacturing cost. Fundamentally, this is realizable by increasing the dielectric
strength of the transformer insulation system [1]. A well-known approach that is typically used in power
transformers is by adding cellulose-based solid insulation, i.e. pressboard between phases of windings [2].
Recently, the use of appropriate nanoparticles with appropriate amount in transformer oil has also shown a
positive impact on the dielectric strength of transformer oil [3].
Generally, a high voltage power transformer comprises the combination of liquid insulation and
cellulose based-pressboard as major insulation in power transformer. The composite insulating system has
raised an issue regarding the surface discharge at the oil-pressboard interface. The oil-pressboard interface is
known as the weak point, involving electric charges deposition and boundaries which can cause the surface
discharge that subsequently lead to the damage of the insulation system [4], [5]. Besides, it is also suspected

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The Correlation between Surface Tracking and Partial Discharge Characteristics … (Nur Amirah Othman)
632
that the discharge initiated at the junction between high voltage electrode and the pressboard insulation is due
to the imperfection of their contact and subsequently lower the creep strength on pressboard surface [6].
Surface discharge or creepage discharge can be categorized into tracking fault which is regarded as
a serious failure mode in large power transformer because it can lead to the catastrophic failure under normal
operating conditions. Tracking is regarded as an electric discharges phenomenon that occur on the solid
insulation leaving the conducting path which is usually observed in the form of carbonized mark and it will
slowly degrade the solid material [6]. It can continue from minutes to months or even years until failure if
there is no proper and effective monitoring on the transformer condition. Figure 1 shows an example of
catastrophic failure along barrier board.
Figure 1. Catastrophic failure along barrier board [7]
Nowadays, the global demand for green technologies is increasing. The efforts towards the
development of environmentally friendly technologies are going on elsewhere in various fields such as
biodiesel [8], gas insulation [9], [10] and solid materials [11], [12]. In the case of liquid insulation, fully
biodegradable vegetable oils (ester oils) have been introduced as potential alternative liquid for the
replacement of mineral oil [13]. The introduction of ester oil should help to reduce the problem of non-
biodegradable mineral oil spillage from ruptured and failure equipment such as transformer that may lead to
the soil contamination. However, until now, the usage of ester oil is quite slow for high voltage power
transformer application due to lack of understanding on the performance of this type of oil especially when
combined with solid material. Therefore, it is important to seek understanding about the dielectric
performance of ester oil-pressboard interface that may exist in large power transformer. This paper focuses
on the study of degradation behavior of surface discharge at the impregnated pressboard immersed in natural
ester oil (MIDEL eN). The surface discharge activity was observed until first appearance of full discharge
and the PD characteristics were analyzed by using phase-resolved partial discharge (PRPD) pattern.
2. EXPERIMENTAL DESCRIPTIONS
2.1. Surface Discharge Experiment
The surface discharge experiment was conducted under sustained AC voltage level of 30 kV for 6
hours of experimental period. This applied voltage was determined in the range between the inception
voltage and breakdown voltage. These inception and breakdown voltages were determined before the surface
discharge experiment was conducted in order to select a suitable voltage level, thus, avoiding immediate
breakdown during a long period of time of surface discharge experiment. For the purpose of partial discharge
measurement, the measured noise level was up to 15 pC. Therefore, by considering +5 pC contingency, a 20
pC of threshold was used throughout the experimental period.
The development of surface tracking on oil-impregnated pressboard surface was correlated between
visual records and the partial discharge data. The OMICRON Mtronix Partial Discharge Measurement
system was used to monitor and record all the PD patterns corresponding to the surface discharge activities
on pressboard surface. A digital camera with ability to capture 60 frames per second (fps) was used to record
all the significant events during surface discharge experiment. Figure 2 shows the experimental setup for the
surface discharge experiment.

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633
Figure 2. Experimental setup for the surface discharge experiment
2.2. Needle-Bar Electrode Configuration
Medical needle with tip radius of 20 µmwas used as a point electrode to initiate the discharge [14].
Medical needle discharge source was placed at an acute angle to the horizontal of the pressboard surface with
a fixed gap distance of 30 mm from the earth electrode [15], [16]. This needle-bar electrode configuration
was used to ensure that the charges built around the needle tip will distribute along the pressboard surface
rather than the bulk of the pressboard [16]. Hence, this will reduce the possibility of the pressboard being
punctured and subsequently can be established and sustained the surface discharge experiment for long
periods of time without electrical breakdown. Figure 3(a) and (b) show the actual image and the dimension
from the side edge of medical needle used in the experiment respectively. The bevel degree (BD), outer (OD)
and inner (ID) diameter and length (L) of the medical needle were labeled.
(a) Actual medical needle type 23G (b) Dimension from side edge
Figure 3. Medical needle used in the experiment
2.3. Pre-processing of Liquid Sample
Natural ester MIDEL eN oil was used as the liquid insulating for the surface discharge experiment.
For the oil treatment process, MIDEL eN oil was dried for 1 hour at 70 and followed by a vacuum
condition of 0.09 MPa for 1.5 hours at 70 . The moisture contents of the oil sample were then measured by
using Karl Fisher titration method. The moisture content of MIDEL eN oil wasbetween 150 – 180 ppm which
was below than the saturation point of moisture content for ester oil, i.e. 200 ppm.
2.4. Pressboard Sample Preparation
New pressboard with a thickness of 2.15 mm, type B.3.1 from IEC 60641-3-1 which is a courtesy of
Malaysian Transformer Manufacturing Sdn. Bhd. (MTM) was used in this experiment. The pressboard
samples were cut into pieces of size approximately 100 mm 100 mm. In this work, 3 % of moisture content
in pressboard samples was used in the study of surface discharge characteristics of MIDEL eN oil-pressboard
interface. This moisture content is expressed as the percentage by weight. In accordance with the standard of
BS EN 60641-2:2004 2004 [17], the pressboard samples were firstly dried in an air circulating oven at 105

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634
for 48 hours. The pressboard samples are considered dry when it is in constant mass at variation of ± 0.5 %
between two successive drying. Afterwards, in order to achieve 3 % of moisture content in pressboard
samples, the samples were then left in the laboratory under atmospheric condition (T = 27 to 31 , RH = 60
to 70 %) until the required mass is achieved from the dried condition. The pressboard samples were then
impregnated in MIDEL eN oil under vacuum condition of 0.09 MPa for 48 hours at 60 [18].
3. RESULT AND DISCUSSION
This section describes the process of surface discharge behavior starting from the beginning of the
experiment until the appearance of first full discharge bridges the gap distance between the needle tip and the
earth electrode without resulting in a complete surface flashover or electrical breakdown. The PD data is also
presented to discuss the PD pattern for each of the stage during surface discharge process.
3.1. Surface Discharge Process at MIDEL eN Oil-pressboard Interface
In the beginning of the experiment, the inttermittent arc discharge was observed instantly as the 30
kV starts to apply. The inttermittent arc discharge wasnormally observed in bluish glow discharge sparking
at the tip of needle electrode. This bluish glow discharge indicates a high field region that sufficiently high
enough for the ionization collisons and secondary anvalanche to take place at the needle tip [19]. This event
may keep repeating up to 5 minutes at the tip of the needle electrode. The typical image of the inttermittent
arc discharge is shown in
Figure 4(a).
After a certain period of time, the white mark starts to develop across the pressboard surface and
form a bush-like shape as shown in
Figure 4(b). This stage was observed and recorded in 5 to 10 minutes after the arc discharge event.
The formation of white mark indicates the drying out of liquid in the pressboard pores through evaporation
and decomposition of oil molecules by the localise heating on the pressboard surface [16], [20], [21].
Consequently, the created gases by the local overheating at the pressboard surface are pushed out from the
pressboard structure by the evidence of small gas bubbles floating out from the pressboard surface into the
surrounding liquid. The formation of small bubbles floating out from the pressboard structure is also due to
the Maxwell’s stress. Based on this concept, the oil that has higher permittivity is capable to push out the
lower permittivity gases from the pressboard structure [21].
Consequently, the discharge drove the extension of white mark slowly with several of branches
spreading halfway across the pressboard surface as shown in
Figure 4(c). Small gas bubbles were rose and floating out from the end of the root of white mark
into the insulating liquid. The thin line of carbonized or black mark was also observed at the vicinity of the
needle tip. Previous research by Zainuddin through his simulation work using finite element method (FEM)
has shown that the surface discharges may cause a significant temperature increase, i.e. beyond 500 K at a
very tiny region which is vicinity to the needle
tip [22]. It is worthwhile noting that such a temperature level may cause carbonization of cellulose through
dehydration and pyrolysis processes [23].
Next, typically after approximately 1 hour of experiment, the track of white mark starts to approach
nearly to the earth bar. At this time, the repetitive bluish arcing was observed at the earth bar and bridge the
track of white mark to the earth bar. The typical image of earth arcing is shown in
Figure 4(d). Some audible crackling with the flashes was also heard during the process. To
elaborate, the charge may accumulate on the pressboard surface due to the charge movement during the
propagation and development of white mark on the oil-pressboard interface which is resulting on the electric
field distribution [24]. The highest point of electric field at the end of the closest point of white mark is
sufficient to cause earth arcing discharge [25]. The repetitive arcing at earth electrode may continue from a
few seconds to minutes due to the some accumulated charges that are still undergo the ionization process at
the oil-pressboard interface during the surface discharge process. Whereas some other accumulated charges
have already transferred to the earth during earth arcing process.
The last process of surface discharge is full discharge event which is temporarily bridges the whole
gap distance from the needle tip to the earth electrode without resulting in a complete surface flashover or
electrical breakdown. The full discharge was occurred when the track of white mark is nearly touched the
earth electrode and subsequently bridges the gap distance by following the white mark track on the
pressboard surface. The subsequent full discharge event can re-occur by following the same white mark track
or another new branch. There are two types of colors that were normally observed during this event which
were in bluish and orange color. The bluish glow was occurred at the earth electrode while the orange glow
was occurred on the pressboard surface following the track of white mark. This finding is similar with the

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previous research in [16]. Most importantly, the full discharge event is totally not the same as the surface
flashover or breakdown. Full discharge is observed as a weak and partial luminous of streamer while surface
flashover is observed as high illumination intensity of streamer with smoky gases [16]. An example of full
discharge event is shown in
Figure 4(e).
(a) Intermittent of arc discharge at the beginning of
surface discharge experiment
(b) Bush-like shape white mark
(c) Propagation of white mark halfway of a gap
distance
(d) Earth arc discharge
(e) Full discharge event
Figure 4. Surface discharge process at MIDEL eN oil-pressboard interface
3.2. Correlation between Surface Discharge Process and PRPD Pattern
Generally, for all data that have been taken, the presence of PD events at first and third quadrants of
AC voltage cycle indicates the surface discharge and corona activies are taking place during surface

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discharge experiment. The PD patterns were also asymmetry between the positive and negative PD amplitude
and phase distribution.
At the beginning of surface discharge experiment (see
Figure 4(a)), the PRPD pattern for this stage is shown in Figure 5. Based on the PD pattern, some of
the PD events were instantly developed across the instantaneous zero crossing of applied AC voltage. At this
instantaneous zero crossing area, even though there is no instantaneous external high voltage stress, the
electric field could still exist to develop the discharge. This is due to the presence of space charge developed
as PD inception voltage is reached that helps to facilitate the discharge activity. This pattern can be observed
throughout the surface discharge experiment.It should be highlighted that this PD pattern is also observed
elsewherein [14].
After a certain period where the propagation of white mark in a bush-like shape (see
Figure 4 (b)), the PRPD pattern starts to change as depicted in Figure 6. Based on the PD pattern,
PD activities broadly spread over the positive and negative half cycle for both first and third quadrants. There
is no significant differences in the PD patterns when the white mark propagate about halfway of a gap
distance
(see
Figure 4(c)) but there is a higher intensity of PD activities that covers a bigger area in both first and
third quarters (comparing Figure 6 and 7).
By comparing the results of PD pattern for the first three stages (see
Figure 4(a-c)), surprisingly, the PD magnitudes (comparing Figure 5-7) seem decrease after
beginning of the experiment until the propagation of white mark is about halfway of a gap distance between
the needle tip and earth electrode
(see
Figure 4(a-c)).The lower PD magnitude during the white mark is about halfway of a gap distance is
might be due to the decreasing of constructive superposition. The decreasing of constructive superposition is
caused by the differences of polarity between external electric field at the needle tip and space charge
accumulation at the interface [25]. The reduction of PD magnitudes during halfway of a gap distance was
also noticed in the previous research [25] which was done using mineral oil. However, the PRPD pattern
recorded using mineral oil was totally different from the ester oil whereby the inception discharge of mineral
oil was clearly displayed at the first quadrant of AC cycle.
Figure 5. PRPD data for a period of 30s at the beginning of surface discharge experiment (associated with
Figure 4 (a))

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Figure 6. PRPD data for a period of 30s during the formation of white mark in bush-like shape (associated
with Figure 4 (b))
Figure 7. PRPD data for a period of 30s during the formation of white mark about halfway of a gap distance
(associated with Figure 4 (c))
Next, Figure 8 shows the typical PRPD pattern obtained during the repetitive bluish arcing at earth
electrode to connect the white mark and bridge the gap distance (see
Figure 4(d)). The PRPD pattern shows that there was high PD magnitude at both peak of positive
and negative half cycles suggesting corona discharge with positive and negative streamers were occurred
during surface discharge experiment. However, the arc discharge was seem cluttering more at peak of
positive half cycle than that the peak of negative half cycle. Therefore, it is suggested that the positive
streamer give more impact on the repetitive arc discharge compared to the negative one. Besides, the high
value of PD magnitude occurring at both peak of positive and negative half cycles is might be due to the high
energy released during the arcing process that ionized the oil molecule. This is evidenced by the bluish arcing
whereby the bluish arc enable to occur in the oil
region [16]. It is also noted that there are PD activities on the first and third quadrants of AC cycle suggesting
surface discharge activity is still on going.

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Figure 8. Earth arc discharge with high magnitude at peak of positive and negative half cycles for a period of
30s (associated with Figure 4 (d))
The repetitive of arc discharge at earth electrode can continue from seconds to minutes and
consequently, the orange glow was observed bridging the electrodes following the white mark track
(see
Figure 4(e)). This event is characterized as a full discharge event which is also observed by
Mitchinson and Zainuddin in their study using mineral oil [15], [16]. Figure 9 shows the PRPD pattern for
full discharge event obtained from the surface discharge process. The discharges distributions are seen
scattered due to the accumulation of space charges drifting toward the earth electrode. The high PD
magnitude observed at both peaks of positive and negative half cycle suggesting the full discharge is a
corona-like event. The density of apparent charge during this event is seen less than 3.0 nC which is less than
that the earth arc discharge process (see Figure 8).
Figure 9. Typical full discharge event occurred during surface discharge process for a period of 5s
(associated with Figure 4 (e))
4. CONCLUSION
A surface tracking experiment has been undertaken to investigate the degradation behavior of
surface discharge on the pressboard surface immersed in MIDEL eN oil by correlating with the PD data.
This work indicated that generally surface tracking on pressboard surface is characterized as a development
of white mark due to the intense discharge at the interface between oil and the pressboard surface. The drying
out process due to the localise heating on the pressboard structure will push out the gases in the pressboard
structure to the surrounding liquid. This event can continue to develop until it bridges the whole gap distance.

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By correlating with the measured data, the results turn out to be not as expected whereby decreasing
in PD magnitude is observed. This decreasing trend is spotted when the propagation of white mark about
halfway of a gap distance which is also observed in the previous study using mineral oil.
ACKNOWLEDGEMENT
Thanks to the Universiti Teknikal Malaysia Melaka and Ministry of Higher Education, Malaysia for
the encouragement and financial support. This work is under Fundamental Research Grant Scheme
(FRGS/1/2014/TK0/FKE/02/F00216). A big appreciation to the Malaysia Transformer Manufacturing Sdn.
Bhd. (MTM) for their courtesy in supplying pressboard.
REFERENCES
[1] S.V. Kulkarni and S.A. Khaparde, Transformer Engineering Design and Practice, 2004.
[2] W. Ziomek, ―Transformer Electrical Insulation‖, IEEE Transactions on Dielectrics and Electrical Insulation, vol.
19, no. 6, pp. 1841–1842, 2012.
[3] M.S. Mohamad, et al., ―Comparative Study on the AC Brekadown Voltage of Palm Fatty Acid Ester Insulation Oils
Mixed With Iron Oxide Nanoparticles‖, International Journal of Electrical and Computer Engineering, vol. 6, no.
4, p. 1481, 2016.
[4] X. Yi, ―Characteristics of Creepage Discharge Along Ester-Pressboard Interfaces under AC Stress‖, PhD Thesis,
University of Manchester, 2012.
[5] P.M. Mitchinson, ―Surface tracking in the inter-phase of large transformers‖, PhD Thesis, University Of
Southampton, 2008.
[6] J. Dai, et al., ―Creepage Discharge on Insulation Barriers in Aged Power Transformers‖, IEEE Transactions on
Dielectric and Electrical Insulation, vol. 17, no. 4, pp. 1327–1335, 2010.
[7] J.A. Lapworth and A. Wilson, ―Transformer Internal Over-Voltages Caused by Remote Energisation‖, in IEEE PES
PowerAfrica 2007 Conference Exposition Johannesburg, South Africa, no. July, pp. 16–20, 2007.
[8] G. Vijaya Gowri, et al, ―Investigation of Neem Fatty Acid Ethyl Ester for Electric Power Generation‖,
TELKOMNIKA Indonesian Journal of Electrical Engineering, vol. 14, no. 1, 2015.
[9] P. Glaubitz, et al., “Sustainable performance of gas-insulated switchgear”, in International Conference on High
Voltage Engineering and Application, pp. 509–513, 2012.
[10] M. Hyrenbach and S. Zache, “Alternative Insulation Gas for Medium-Voltage Switchgear”, in Petroleum and
Chemical Industry Conference Europe (PCIC Europe), pp. 1–9, 2016.
[11] R. Zhang and C. Chen, ―Intelligent Green Production of raw materials in ceramic technology of choice‖, in
International Conference on Electronic & Mechanical Engineering and Information Technology, pp. 0–3, 2011.
[12] A. Aman, et al., ―Polymeric composite based on waste material for high voltage outdoor application‖, International
Journal of Electrical Power & Energy Systems, vol. 45, no. 1, pp. 346–352, 2013.
[13] Martin J. Heathcore, CEng, and FIEE, J&P Transformer Book. 2007.
[14] X. Yi and Z.D. Wang, ―Surface Tracking on Pressboard in Natural and Synthetic Transformer Liquids under AC
Stress‖, IEEE Transactions on Dielectric and Electrical Insulation, vol. 20, no. 5, pp. 1625–1634, 2013.
[15] H. Zainuddin, et al., “Partial Discharge Characteristics of Surface Tracking on Oil-impregnated Pressboard under
AC Voltages”, in IEEE International Conference on Solid Dielectrics, Bologna, Italy, June 30 – July 4, 2013 It, pp.
1016–1019, 2013.
[16] P.M. Mitchinson, et al., ―Tracking and Surface Discharge at the Oil-Pressboard Interface‖, IEEE Electrical
Insulation Magazine, vol. 26, no. 2, pp. 35–41, 2010.
[17] BS EN 60641-2:2004, ―Pressboard and presspaper for electrical purposes — Part 2: Methods of tests‖, 2004.
[18] J. Dai and Z.D. Wang, ―A Comparison of the Impregnation of Cellulose Insulation by Ester and Mineral oil‖, IEEE
Transactions on Dielectrics and Electrical Insulation, vol. 15, no. 2, pp. 374–381, 2008.
[19] D. Linhjell, et al., ―Streamer propagation under impulse voltage in long point-plane oil gaps‖, IEEE Transactions
on Dielectrics and Electrical Insulation, vol. 1, no. 3, pp. 447–458, Jun. 1994.
[20] V. Sokolov, et al., “Effective Methods Assesment of Insulation System conditions in Power Transformers : A View
Based on Practical Experience”, in Proceedings of the Electrical Insulation Conference and Electrical
Manufacturing & Coil Winding Conference, Cincinnati, Ohio, USA, pp. 659–667,1996.
[21] F. Murdiya, et al., ―Creeping discharge developing on vegetable-based oil / pressboard interface under AC
voltage‖, IEEE Transactions on Dielectrics and Electrical Insulation, vol. 21, no. 5, pp. 2102–2110, Oct. 2014.
[22] H. Zainuddin and P.L. Lewin, “Modeling of Degradation Mechanism at the Oil-Pressboard Interface due to
Surface Discharge”, in COMSOL Confference, 2015.
[23] D.F. Arseneau, ―Competitive reactions in the thermal decomposition of cellulose‖, Canadian Journal of Chemistry,
vol. 49, pp. 632–638, 1971.
[24] N. Inoue, et al., “Mechanism of Charge Accumulation at Flowing Oil/Pressboard Interface Based on Optical
Measurement of Electric Field”, in Annual Report Conference on Electrical Insulation and Dielectric Phenomena,
pp. 536–539, 2001.
[25] H. Zainuddin, ―Study of Surface Discharge Behaviour at the Oil-Pressboard Interface‖, PhD Thesis, University Of
Southampton, 2013.

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BIOGRAPHIES OF AUTHORS
Nur Amirah Othman received the Bachelor degree in Electrical Enginering (Control,
Instrumentation and Automation) from Universiti Teknikal Malaysia Melaka (UTeM) in 2014.
She is currently pursuing her MSc in Electrical Engineering at UTeM. Her research focuses on
monitoring the condition of partial discharge in high voltage insulation.
Hidayat Zainuddin received his Bachelor of Engineering in Electrical from the Universiti
Teknologi Malaysia in 2003. He obtained his MSc in Electrical Power Engineering with Business
from the University of Strathclyde, Glasgow in 2005. He received his Ph.D degree at the
University of Southampton in 2013. He has been as academic staff of the University Teknikal
Malaysia Melaka since 2003 and at present is the senior lecturer in the Faculty of Electrical
Engineering at the university. He was the Manager of Centre for Robotics and Industrial
Automation, University Teknikal Malaysia Melaka from 2014-2016. His research interests
include HV equipment and insulation condition monitoring, failure analysis, and power system
protection coordination.
AminudinAman was born in Melaka, Malaysia in 1973. He received his B. Eng., Master
Degree and PhD from University of Technology Malaysia in 1998, 2007 and 2013 respectively,
in Electrical Engineering. His employment experience starts in 1998 as an Electrical Engineer at
the industry. At present he is serving as Senior Lecturer and holding a post of Head of
Department for Industrial Power Department in Universiti Teknikal Malaysia Melaka. His
special fields of interest included the high voltage solid insulation and high voltage engineering.
Sharin Ab Ghani received the B.Eng.(Hons) degree in Electrical Engineering from Universiti
Teknikal Malaysia Melaka in 2008 and the M.Eng. degree in Electrical Engineering from
Universiti Tenaga Nasional, Malaysia in 2012. He served as a lecturer at Universiti Teknikal
Malaysia Melaka. Currently he is a PhD student at Universiti Teknologi Malaysia. His research
interests are in electrical insulation, power equipments & insulation condition monitoring, and
renewable energy.
Imran Sutan Chairul received the BSc. (Hons) in Electrical Engineering (Industrial Power)
from Universiti Teknikal Malaysia Melaka (UTeM) in 2008. In 2012, he received the Master of
Electrical Engineering from Universiti Tenaga Nasional. Currently, he is a lecturer at Universiti
Teknikal Malaysia Melaka (UTeM). His research interests include liquid and gas insulation as
well as condition monitoring of power transformer.

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