S1-G2 FinalReport HVE
S1-G2 FinalReport HVE
PROJECT REPORT
GROUP MEMBERS:
NO NAME MATRIC NUMBER
SECTION: 1
NAME OF LECTURER:
Prof. Madya Dr. MD NOR RAMDON BIN BAHAROM
ABSTRACT
In this project, the students designed an insulator which is often used in overhead
line towers. This insulator is used to separate electrical conductors without allowing current
to pass through them, and it also serves as a safety measure during maintenance.
Insulators for overhead lines are essential for a power system's operation. Poles or towers
are needed to support the overhead line cables. Line conductors must be appropriately
insulated from supports to avoid current flowing to the ground. The insulator protects the
transmission line from overvoltage produced by lightning, switching, or other crucial
conditions. Glass surface of the glass insulator has high mechanical strength, the surface
is not easy to crack. Then, a suitable creepage clearance distance needs to be suitable
with the level of pollution.
The purpose of this project is to develop a suspension type overhead line insulator as well
as simulate and analyse the normal voltage and electric field distributions on the prototype.
The insulator property and capability will be analysed and tested utilising Finite Element
Method Magnetics (FEMM) Software. It's created with 3D drawing tools such SketchUp,
and the material for the insulator is chosen. Because the system voltage is 132kV, we
used insulator properties such as suspension string as the type of insulator, glass as the
insulator material, and cap and pins as fittings. The findings of the study are based on
overhead line insulator theory, as well as an analysis of the best materials for each
situation in terms of electrical and mechanical properties, environmental performance,
costing, and the advantages and disadvantages of the chosen prototype.
1.0 COMPANY INFORMATION
1.1 COMPANY BACKGROUND
1.1.1 INTRODUCTION
Empire Power Engineering (EPE) Sdn Bhd is located in Parit Raja, Batu Pahat,
Johor. This company was established in January 2020 as an Electrical and Mechanical
Contractor. The main goal of this company is to meet the needs of the construction
industry as a capable and competent firm. With exceptional experience, capabilities and
skills, it is necessary to achieve and meet all project requirements to the highest standards.
These different abilities are developed over time working as a team, primarily to maintain a
consistent high standard of work.
The company is steadfastly committed to giving team projects and full team
support top priority when working on projects. Empire Power Engineering (EPE) Sdn Bhd
has always prioritised the use of resources, machinery, and materials as part of its
corporate philosophy. Every project undertaken will be guaranteed and delivered on time
with the application of a strict quality assurance plan. Additionally, the business offers
premium materials at affordable prices.
Empire Power Engineering (EPE) Sdn Bhd is confident that with the current team,
the company can complete projects on schedule and to the satisfaction of the customer
given its experience and management skills in understanding customer needs.
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1.1.2 COMPANY VISION
“We will make electricity so cheap that only the rich will burn candles”
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1.1.6 COMPANY ORGANIZATION CHART
DIRECTOR
NITHIYAAN A/L RAJA
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1.2 PROJECT INTRODUCTION
Transmission lines are primarily exposed to nature's hostile climate in the air, which
causes a variety of issues. Thunder, rain, lightning, flashover, winter ice, fog, fog stick on
the insulator, and pollution all contribute to poor contact insulators and transmitters. The
support tower is separated from the conductor by an insulator, which is a nonconductive
material. The quality of the insulator will deteriorate over time as a result of contamination
in the surrounding environment. Contamination effects are a type of pollution that occurs at
the surface of the insulator as a result of the natural environment or factory smoke. The
contamination effect can cause overhead transmission line failures such as faults, corona
effect, and flashover. This project is designed to investigate the electrical performance of
the surrounding insulator in relation to the available options. As a result, the primary goal
of this project is to design and test the performance of insulator string in both clean and
contaminated environments.
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1.2.2 OBJECTIVES
3. Able to simulate the HV and EM fields distribution and analyse the performance
of the prototype when stresses by environmental impact.
1.2.3 SCOPES
3. Glass has been chosen as the insulator for this investigation. For both types of
insulators, the data is evaluated using COMSOL Multiphysics software's Finite
Element Method (FEM), and the comparison is observed and analysed.
2. Able to draw the proposal designs professionally using 2D/3D drawing software
such as SketchUp.
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2.0 DESIGN PLANNING
In term of designing and selecting suitable components and value, there are a few
studies related to the glass insulator as the insulator for transmission line grid. Toughened
glass insulators have advantages such as steady mechanical strength, self-exposure of
faults, and so on, which offset disadvantages such as tedious insulation resistance
detection in porcelain insulators, fast ageing of composite insulators, and easy string
falling. Since its introduction into the power grid, it has sparked widespread interest, with
disc suspension glass insulators accounting for up to 70% of transmission line insulators
[1] . High voltage tests were conducted on a batch of aged transmission line glazed glass
cap and pin insulator to measure the insulator self-capacitance, surface resistance, critical
flashover voltage and corona inception voltage in order to evaluate transmission line
insulator [2].
Cap and pin insulator is taken as research object with contaminant layer are
modelled on the surface of the insulator. This distorted field will expedite the premature
aging process that may lead to flashover and result in power system network interrupted. It
is believed that the calculated field would help in improving the insulator design especially
for contaminated areas with various climates [3] . Rainfall decreases insulator
contamination, which is linked to the electrical performance of high-voltage transmission
line outside insulators because it minimises the possibility of pollution flashover. An
artificial rainfall experiment platform was devised, manufactured, and tested to investigate
the washing effect of rainfall on contamination of porcelain and glass insulators. It has the
ability to alter rainfall strength, flushing angle, duration, and homogenous. Suspension
insulator string rain experiments have been conducted. Comparison of experimental
results shows that the effect of rainfall's flushing angle on washing insulators'
contamination is the biggest, next is rainfall's intensity, and the minimal is rainfall's duration
[4].
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3.0 ANALYSIS OF PROPOSAL DESIGN
3.1 CONCEPT OF THE DESIGN
The number of suspension glass discs insulator that have been design can be
calculated by using the formula below:
Formula:
𝑉𝐿
𝑁= + 𝑆𝑓
3 × 11
Where:
𝑁 = 𝑁𝑢𝑚𝑏𝑒𝑟 𝑜𝑓 𝑠𝑢𝑠𝑝𝑒𝑛𝑠𝑖𝑜𝑛 𝑔𝑙𝑎𝑠𝑠 𝑑𝑖𝑠𝑐𝑠 𝑖𝑛𝑠𝑢𝑙𝑎𝑡𝑜𝑟
𝑉𝐿 = 𝑆𝑦𝑠𝑡𝑒𝑚 𝑣𝑜𝑙𝑡𝑎𝑔𝑒 (𝑖𝑛 𝑘𝑉)
𝑆𝑓 = 𝑀𝑒𝑐ℎ𝑎𝑛𝑖𝑐𝑎𝑙 𝑠𝑎𝑓𝑒𝑡𝑦 𝑓𝑎𝑐𝑡𝑜𝑟 (𝑈𝑠𝑢𝑎𝑙𝑙𝑦 𝑡ℎ𝑒 𝑣𝑎𝑙𝑢𝑒 𝑜𝑓 𝑆𝑓 𝑖𝑠 1 𝑜𝑟 2)
Therefore, we consider 𝑆𝑓 = 1
Calculation:
𝑉𝐿
𝑁= + 𝑆𝑓
3 × 11
132
𝑁= + 𝑆𝑓
3 × 11
𝑁 ≈ 7 + 𝑆𝑓
𝑁 ≈ 7+1
𝑁=8
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3.1.2 CREEPAGE CLEARANCE
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3.2 2D & 3D
DRAWING
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Figure 3: 3D insulator Design
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Figure 4: 2D and 3D stacking insulator design
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3.3 MATERIAL PROPERTIES
Based on its benefits, it was chosen to apply stacked insulator string, which is a
suspension type overhead line, for this project. The following are some of the
benefits of stacked insulator strings:
1. Suspension type insulators give more flexibility to the line and mechanical
stresses due to wind and other factors are reduced in this suspension type
insulator arrangement.
3. Suspension insulators are cheaper in cost compared to pin type insulators for
operating voltage above 50kV
The material used for the design insulator is glass. Glass is a material that has high
dielectric strength that can insulate conductive material which is efficient for high
voltage conductors. The advantage that glass material has as an insulator is stated
below:
1. Surface of the glass insulator has high mechanical strength, the surface is not
easy to crack.
2. It has a very long service life, because the mechanical and electrical functions
of the glass are not affected by aging.
3. The use of glass insulators can eliminate the routine preventive testing of the
insulators during operation.
4. The raw materials used to manufacture glass insulators are more stable
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3.4 ELECTRICAL CHARACTERISTICS
The method for determining the strength rating of composite and ceramic insulators is the
same. A composite insulator can immediately replace porcelain or glass insulators based
on strength alone. The strength rating of composite insulators is defined in table 3.
Because all materials have a time-load characteristic that reduces their residual strength
over time, a two-to-one safety factor has traditionally been utilised when selecting an
insulator's strength rating. Composite insulators are typically rated at a maximum working
load of 50% of the Ultimate Load rating.
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Insulators are often made of toughened glass. To make the shell, melted glass is poured
into a mould. The shells are cooled by dipping into hot and cold baths.
This thermal treatment shrinks the glass's surface and puts pressure on the body,
increasing the glass's mechanical strength. The glass will break into little fragments if
exposed to sudden mechanical pressures, such as a hammer blow or bullets. Alumina
cement is used to secure the metal end-fitting.
Figure 5: Transmission Line Tower at Kolej Kediaman Bestari (KKB) Parit Raja, Batu
Pahat
As shown in the figure 5 above, the location chosen for this project is at Kolej
Kediaman Bestari (KKB) Parit Raja, Batu Pahat. This area consists with average number
of houses and is several kilometres from the nearest coastal area which is Pantai Minyak
Beku. This location of the project is also subjected to frequent winds and/or rainfall. This
area also consist of industries not particularly producing polluting smoke.So, the design of
the suspension type insulator proposed will be implemented at this location which can be
said with medium level of pollution.
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4.0 TECHNICAL SUMMARY METHODOLOGY OF FEA SIMULATION SOFTWARE
Procedures and techniques for simulating the project to build that the appropriate
results and data can be collected and analysed. There are a few things to think about
before starting the simulation process. The students in each group must choose the
insulators that will be tested. Research and study of material characteristics are required
before deciding the type of insulator.
Next, the partial differential equation can be solved numerically by meshing the
model. When geometry is broken into smaller units known as elements, linear behavior
can be assumed for each unit, which can then transform the entire system into a system of
linear equations stated by a matrix and solved by software to get the closest approximation
to the system equation. In essence, meshing the model converts it into a set of linear
equations that can be used to resolve the electrical issues. The best way to produce a
more accurate result is with a finer mesh, but the disadvantage is that it takes more time to
compute.
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5.0 WORKFLOW FEA SIMULATION ON THE PROTOTYPE
This project uses a cap-and-pin fitting with a 132 kV system voltage. Toughness
glass was used as the insulator material in a contaminated environment. The insulating
component of this project has 2 size that with a diameter of 172 mm and 141 mm, and a
creepage distance of 400 mm and 320 mm. Based on the toughness glass material, the
relative electric permittivity values for the material characteristics are 10 and the values of
electric conductivity (S/m) is 0 while the steel conductor has 1100000 relative permittivity
with 132000 voltages. The standard and data profile of toughness glass insulator as well
as steel conductor also must be studied. Then, we had to build a geometry. The insulator
that we chose is the prototype that we are going to simulate in FEMM. It can be in
cartesian or planar and it should be in 2 dimensions (2D). For our group, we sketch the
insulator in 2D by using FEMM simulation software.
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7.0 SIMULATION
Figure shows the field intensity of a big size of single disc glass insulator in a dry condition.
The field intensity at the bottom of the disc more focused and higher at the steel pin that is
connected to the 11 kV high voltage terminal. It is only connected to 11 kV because this is
only the single disc and not stacked yet.
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Figure 8: Field intensity simulation of big size single disc insulator for dry test
Figure shows the electric potential of a single disc insulator that is measured from
the high voltage side. From the graph, the electric potential is constant until around 80 mm
and starting to drop to 0V at around 130-140 mm.
Figure 9: Graph of voltage versus length for big size single disc insulator
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Figure shows the field intensity graph of the single disc insulator starting to spike at
around 80-90 mm at more than 30000 V/m and slowly dropping below than 200000 V/m
before drop to 0 V/m at around 130-140 mm.
Figure 10: Graph of field intensity versus length for big size single disc insulator
Figure shows the field intensity of the small size glass insulator where the focused
and more intense area are quite similar to the big size of glass insulator for dry condition.
The field more intense at the bottom of the insulator at the area of steel pin and small
intensity at cap steel area.
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Figure 11:Mesh model of the small size single insulator for dry test
Figure 12: Field intensity simulation of small size single disc insulator for dry test
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Figure shows the electric potential graph for small size of disc insulator in dry
condition. The value of initial electric potential is constant at 11 kV from 0 mm before
starting to drop slowly until 0 V from 90 mm until around 160 mm.
Figure 13: Graph of voltage versus length for small size single disc insulator
Figure shows the field intensity of the small size of the glass insulator disc. The field
intensity on this glass did not have a sharp turn as the big size glass insulator as this
insulator move smoothly to the peak of intensity level before going down to zero at the end
of insulator.
Figure 14: Graph of field intensity versus length for small size single disc insulator
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7.1.3 Stacked Disc Insulator (Dry Test)
The figure below shows the field intensity of the stacked glass insulator in a dry test. The
above level and the bottom level of the insulator has been zoomed in to give a clear
information of the results of the simulation. The below level of the insulator shows the high
intensity field of 132 kV and at the end of the stacked insulator which is the top level of
insulator, it shows that there is no more field intensity at the area showing that the stacked
insulator has a good insulation.
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Figure 16: Field intensity simulation of stacked disc insulator for dry test
Figure 17 and Figure 18: Zoom in view for the stacked disc insulator in dry condition
The both graphs below show the electric potential graph and the field intensity graph of the
stacked glass insulator. The electric potential shows that the voltage from 132 kV
decreasing slowly until reaching 0V at the end of the insulator giving the information that
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this insulator could prevent the electric potential to get pass through. The field intensity at
the beginning of the insulator spike quite high and then slowly decreasing along the
insulator at the end of the insulator.
Figure 19: Graph of voltage versus length for stacked disc insulator in dry condition
Figure 20: Graph of field intensity versus length for stacked disc insulator in dry condition
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7.2 WET TEST
The simulation for wet test at big glass insulator showing that the field intensity of
the glass insulator while in wet condition is a little bit higher than in dry condition with
almost 400000 V/m of intensity field. But for the electric potential, the value remains the
same at 11 kV does not matter in wet or dry condition. The electric potential and the field
intensity are still decreasing after a certain distance until reaching the 0 level.
Figure 21: Mesh model of the big size single insulator for wet test
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Figure 22: Field intensity simulation of big size single disc insulator for wet test
Figure 23: Graph of voltage versus length for big size single disc insulator
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Figure 24: Graph of field intensity versus length for big size single disc insulator
The figure and graphs below show the simulation of small glass insulator in wet
condition. The field intensity of the small glass insulator shows that the value is a little bit
higher than the insulator while in dry condition at almost 300000 V/m while the electric
potential are remains the same as dry condition which is 11 kV. The value of both are
decreasing after a certain length of insulator.
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Figure 25: Mesh model of the small size single insulator for wet test
Figure 26: Field intensity simulation of small size single disc insulator for wet test
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Figure 27: Graph of voltage versus length for small size single disc insulator
Figure 28: Graph of field intensity versus length for small size single disc insulator
The figure and graph below show the simulation of the stacked glass insulator in
wet condition. The field intensity shows there is a spike when going through the steel and
the value of half of the insulator hit the same high of intensity. And going to 0 at the end on
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each insulator. The electric potential of the insulator in wet condition is seems to have a
similar value as the dry test at 132 kV. Both of the electric potential and field intensity are
going to zero after certain length of insulator.
Figure 29: Mesh model of the big size single insulator for wet test
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Figure 30: Field intensity simulation of stacked disc insulator for wet test
Figure 31 and Figure 32: Zoom in view for the stacked disc insulator in wet condition
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Figure 33: Graph of voltage versus length for stacked disc insulator in wet condition
Figure 34: Graph of field intensity versus length for stacked disc insulator in wet condition
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7.3 Comparison Between Dry Test and Wet Test
7.3.1 Comparison Between Dry Test and Wet Test Big Size Single Disc Insulator
Figure 10 and figure 24 shows the graph of field intensity versus length for big size
single disc insulator. From the figures, it could be seen that the insulator when be done
wet test at figure 24 have a higher intensity than the insulator when it in dry condition.
7.3.2 Comparison Between Dry Test and Wet Test Small Size Single Disc Insulator
Figure 14 and figure 28 shows the graph of field intensity versus length for small
size single disc insulator. From the figures, compare to the big insulator the graph the
small insulator insulator have more vibrating than the big insulator. It also could be seen
that the insulator when be done wet test at figure 28 have a higher intensity than the
insulator when it in dry condition.
7.3.3 Comparison Between Dry Test and Wet Test Stacked Disc Insulator
Figure 20 and figure 28 shows the graph of field intensity versus length for stacked
disc insulator in dry condition average initial intensity level, in wet condition are higher than
the dry condition of the insulator.
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Faculty of Electrical and Electronic Engineering
Email: - de190107@siswa.uthm.edu.my
For continuous periods of experimentation only. Re-validation of this document is required for
breaks in experimentation greater than one month or when test circuit is dismantled and re-
assembled.
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SACTION TO EXPERIMENT
Name of the student: Muhammad Hanif Aiman Bin Signed: Hanif Date: 23 June
Samsul Bahri
Name of the supervisor: ASSOC. PROF. Dr Md Nor Signed: Dr Ramdon Date: 23 June
Ramdon bin Baharom
*HoL must be identified and sign here having confirmed the safety documents to be satisfactorily
completed.
Signature: Dr Ramdon
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METHOD STATEMENT
APPENDIX A
HVDC generator
Glass insulator
Earthing rod
Nozzles
DC voltmeter
Control panel
C. Experimental Procedure:
1. For contamination test, the insulator was energized with both positive and negative
polarities of the applied voltage
3. Repeat process for five times to get the average breakdown voltages.
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RISK ASSESSMENT
Title Of Experiment / Test: - HVDC with and without contamination test Date: - 22 June 2022
Prepared By: - Arif Zuhdy bin Validated By: - PM Md. Dr. Ramdon Checked By: - PM Md. Dr. Ramdon bin
Zullkela bin Baharom Baharom
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(In addition to this risk assessment, a safety commissioning checklist is attached to this document. This checklist is to be completed before HV
supplies can be energised. It is relevant to the ‘Electrical shock from high voltage’ and ‘Fire’ hazards described in the table below.
Hazard (s) & Persons or Equipment at Risk Control measures applied to eliminate / minimise
Risk Acceptable?
Possible risk
Risk rating
Likelihood
Severity
Consequences
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All leads leaving from cage have earthed sheath
(current measurements taken at earthed end of
sample, voltage measurement taken with commercial
voltage probe)
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initially operated to confirm behaviour of samples
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RECORD OF CHEMICAL USAGE WITHIN EXPERIMENT
- - - - -
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HAZARD CHECKLIST
You should indicate the hazards present in the experiment in the table below. If a hazard is present,
control measures should be stated on the risk assessment. Note that this list is not exhaustive.
Tripping Hazards X
Slipping Hazards X
Fire X
High Temperatures X
Low Temperatures X
High Pressure X
Low Pressure X
Chemical Spillage X
Working At Height X
Manual Handling X
Production/Use Of Radiation X
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RISK ASSESSMENT SEVERITY MATRIX
Severity
1 2 3 4 5
1
Likelihood
44
5
6–8: Medium: Review, introduce further controls to reduce to as low as reasonably possible
9–25: High: Intolerable. Do not commence work, further control measures required
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HV TESTING PROPOSAL: CODE OF CONDUCT
The safety measures for the person conducting measurements on high voltage or
high-power sources of various types, such as power system lines, direct voltage
supplies, and lighting impulse generators, are discussed in this suggested HV testing.
The electrical hazard associated with temporary measuring rather than metering,
relaying, or normal line operations is addressed by this recommended practise. The
recommended practises are based on the IEEE Recommended Practices for High-
Voltage and High-Power Testing as well as other studies.
Testing Information
The majority of the time, outdoor insulators are contaminated by a variety of sources.
Pollution has become a serious threat to the insulation of power networks in some
areas. Dry contaminants will not be a problem on the insulating surface. On the
insulator surface, wet contamination is a major problem. Moisture in the form of light
rain moistens the pollution layer on the insulating surface. A pollution test can usually
be carried out in one of two ways. The first test is for natural pollution, and the
second is for man-made pollution. The insulator is powered to its operating voltage
and exposed to a naturally polluted environment while its performance is monitored
in a natural pollution test. An artificial pollution test has been devised by simulating
one of the natural weather conditions that causes pollution flash-over.
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Schematic Diagram
The test setup for polymeric insulators at the High Voltage Laboratory is depicted
schematically in Figure 35. The test determines the resistance of the insulation
sample to electrical stress induced by positive and negative impulse voltages. An
impulse generator set provides either positive or negative impulse voltages to the
test circuit, and a capacitor divider monitors the output voltage. Positive lightning
impulses, as well as wet and dry conditions, were used to test polymer insulators to
see if they could withstand 132kV. Artificial rain is created using fog nozzles that
completely cover the sample surfaces. It complies with the criterion in terms of
conductivity and flow rate. It's used to produce pollution by conducting wet flashover
tests on insulators. Each test is subjected to voltages for about one to three minutes.
During the dry condition test, no artificial rain is applied to the sample surface. When
a voltage is supplied to a specimen during dry and wet testing, data is collected by
current and voltage measurements, visual corona creation on fittings/surfaces,
flashover, damage occurrence, and other methods.
Test Setup
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light lamp lights the room when the supply is turned on, and danger signs are put on
the wire mesh to warn against unauthorized entry.
Apply the test voltage for one to three minutes after making all of the necessary
connections. The time interval is a standard in the industry that allows all readers to
take the reading at the same time. As a result, reading comparisons will be
informative because the test procedures are consistent, even though different people
take them. During this time, the resistance should drop or remain roughly constant.
The resistance value should be read and recorded after one minute. In hard
installation situations, such as those with temperature extremes and/or chemical
contamination, this process is expedited. This deterioration has the potential to
jeopardise power dependability as well as personnel safety. As a result, it is
essential to detect this deterioration as soon as possible in order to take corrective
action.
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Details about safe ways of work for testing activities should be provided wherever it
is reasonably practical. All personnel should be involved in the development of safe
work systems in order to produce a workable system. When testing is confined to
diagnostic testing by electrically qualified employees on electrical distribution
systems and equipment (e.g., switchgear), the written records should include the
core safe operating principles.
4. What type of power supply should be used to power the equipment under test,
especially if doing so incorrectly could compromise safety.
5. What is expected of test staff in terms of pre-use inspection of test equipment and
how faults should be notified; (g) the appropriate operation of any warning devices
employed as part of the authorised test site's safety system.
Permanent test sites should be encircled by walls or some other physical barrier.
Because the gates are open, no test voltage should be applied to these areas.
Outside the gates, vital warning signs such as DANGER—HIGH VOLTAGE should
be displayed.
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2. TEMPORARY TEST AREA
II. Brightly coloured safety tape, approximately waist high, installed to suitable safety
signs. After the test has been completed and the test voltage has been withdrawn,
the tape must be removed before anyone can access this area. One or more
observers must be stationed to monitor the entire area if the operator lacks a
comprehensive view of the taped-off section. Never leave a taped-off area
unattended while using test power.
3. INTERLOCK SYSTEMS
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The COSHH Regulations provide a framework for protecting workers' health against
hazards posed by job tasks that expose them to hazardous substances. A COSHH
assessment outlines the safety precautions that must be taken to avoid injury.
Unfortunately, there is a common misconception that risk assessment is the process
of determining a substance's hazardous features; hazardous properties refer to a
substance's ability to cause harm, whereas risk refers to the likelihood of injury under
actual use settings.
Assessors must be able to distinguish between these two concepts. The purpose of
a chemical risk assessment (the COSHH assessment) is to ensure that an educated
decision is made about the control measures that should be adopted to prevent or
restrict exposure to hazardous substances. A risk assessment, in practise, reveals
that suitable and sufficient judgement was employed to arrive at these conclusions.
Consumers can use safety data sheets to analyse the risks associated with chemical
commodities. They describe the chemical's risks and provide directions for handling,
storage, and emergency reaction in the event of an accident.
In the pollutant performance testing, silicone rubber insulators were used. The IEC
insulator test protocol is used to conduct artificial pollution testing. The studies are
set up to mimic real-life scenarios.
Insulators are commonly used to separate the conductor from the pole in electrical
power transmission systems. Its purpose is to stop current from passing from a
conductor to the earth. Before employing the insulator, some parameters must be
examined. Insulator testing requires two types of electrical tests: wet flashover (a
one- to three-minute rain test) and dry flashover (one minute to three- minute dry
test).
In the dry state, the test object is exposed to a high-frequency voltage. The power
voltage is boosted to the stated voltage rating of the insulator plate. This voltage
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rating is kept for a set amount of time. The voltage is increased after one minute till
the flash happens. This method needs to be done five times. It is calculated the
average flashover voltage of the five flashes. The average voltage must not be less
than the power frequency's value.
Artificial rain is required to create a realistic rainy environment around the insulator.
A test voltage is applied to the insulator for a set amount of time, and rain can fall on
it. The voltage is raised to the point where there is a flashover. Voltage is provided
again after a few seconds. To calculate the average flashover voltage, repeat the
method five times more. The average voltage must not be less than the application's
stipulated wet flashover voltage.
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8.0 CONCLUSION
There will be various improvements made to the insulator version in the future to
improve the resistiveness to high voltage, which will be valuable for learning and
teaching approaches. The significance of increasing creepage and giving the
insulator impact follows next. Because the insulator material will be reduced while
the space between a conductive portion and the equipment's bounding surface will
be increased. In general, the design of this insulator was based on preparatory
theoretical research and understanding of dielectric materials gathered through
lecture courses and notes. The majority of the study was conducted using books,
with extra information coming from the internet and publications.
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9.0 REFERENCES
[1] C. Yafeng, Y. Yi, Z. Liu, X. Zhiqiang, Y. Yishi, and L. Zhenyu, “Analysis and
Suggestion on String Breakage Failure of Glass Insulator in 500kV Transmission
Line,” 2020. Accessed: May 10, 2022. [Online]. Available: https://ieeexplore-
ieee-org.ezproxy.uthm.edu.my/document/9279573/
[2] H. Ahmad et al., “Evaluation of transmission line insulator for I-Type string
insulator design,” PECON 2016 - 2016 IEEE 6th International Conference on
Power and Energy, Conference Proceeding, pp. 50–53, Jun. 2017, doi:
10.1109/PECON.2016.7951471.
[5] Glushkov, Daniil A.; Khalyasmaa, Alexandra I.; Dmitriev, Stepan A.; Nikonov,
Ivan P.; Zinoviev, Kirill A. (2014). Polymeric Insulation: Advantages and
Disadvantages. Advanced Materials Research, 1008-1009(), 615–619. doi:
10.4028/www.scientific.net/AMR.1008-1009.615.
[7] A. Banik, S. Dalai, and B. Chatterjee, “Studies the effect of Equivalent Salt
Deposit Density on leakage current and flashover voltage of artificially
contaminated disc insulators,” 2015 1st Conference on Power, Dielectric and
Energy Management at NERIST (ICPDEN), 2015.
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[8] A. Bojovschi, T. Quoc, H. Trung, D. Quang, and T. Le, “Environmental Effects on
HV Dielectric Materials and Related Sensing Technologies,” Applied Sciences,
vol. 9, no. 5, p. 856, 2019.
55