INTERNATIONAL CONFERENCE ON ELECTRIC POWER ENGINEERING (ICEPENG 2015) OCTOBER 14-16, 2015
High Voltage Engineering Practice: A Vehicle for Enhanced National Grid Performance L. C. EKECHUKWU PhD, MNSE
T. C. MADUEME PhD, MNSE, MNIEEE
NEWS ENGINEERING (NIG) LTD. ABUJA, NIGERIA.
[email protected]
DEPT. OF ELECTRICAL ENGINEERING, UNIVERSITY OF NIGERIA, NSUKKA, NIGERIA.
[email protected]
Abstract-The grid system is a configuration of generating stations, high voltage transmission, sub-transmission, and distribution lines, with all their associated auxiliary elements, insulations, communication networks and protective gears. The entire length is interrupted at various points known as transformer stations for the purpose of voltage transformations, in conformity to the designed grid configuration. The safety, reliability and efficiency of power delivery rest on the quality of the associated dielectrics alongthe lines and substations. This paper is aimed at highlighting the importance and roles of quality insulation and dielectrics in power system grids. Philosophy of some dielectric tests and measurements such as insulation resistance, polarisation index (PI), breakdown voltage (BDV), tangent (loss angle) delta(δ), are illustrated for the comprehension of import and applications of High Voltage Engineering (HVE) practice for a reliable grid performance. Capacitor characteristics and similarity in system dielectrics are examined. Types and significance of some vital high voltage tests are mentioned. Results of conducted tangent delta (δ) tests on a 132/11 kV, 63 MVA transformer bushings of the Ajaokuta integrated Steel Plant, Ajaokuta, Kogi State, Nigeria are presented and analysed with reference to the manufacturer’s limits. The test results substantiate high voltage engineering practice as an indispensable vehicle for an efficient grid performance. Key Words: High Voltage, Grid, Dielectrics, Capacitance, Leakage Current, Insulation resistance, Tests
I.
INTRODUCTION
While Thomas Alva Edison (1847 – 1931) patented low voltage discovery and supply through a very limited distance, with voltage drop constraints, Nikola Tesla (1856 – 1943)conceived the concept of alternating
transmission and transfer capability P in an AC system are the following: (1)
P = V2/Z
(2) Where S, the apparent power is in kVA, V the
line-to-line voltage is in Kilovolts (kV),I the line current in Amperes (A), and Z, the wave impedance of a transmission line is in ohms. This equation clearly shows that transmission of a fixed amount of Kilovolts Amp (kVA) over a transmission line, at a preferable higher voltage, is accompanied with a corresponding lower current, for a balanced power transfer. Table 1 shows the relationships between a typical power transfer capability of an alternating current (AC) system, operating voltage and transfer distance.
Table 1 Power Transfer Capability of An AC System And Its Relationship With Operating Voltage And Transfer Distance 220 330 500 750 1000 V, (kV) 256 250 Z, (Ohms) 400 303 278 121 360 900 2200 4000 P, (MW) 100 200 Around ˃ ˃ Transfer – – 1000 1000 1000 Distance, 300 600 (km) Source [2]
current in 1886, alongside using transformers for voltage
Lower currents are highly advantageous, as the watt
step-up, thereby reducing proportionally the line current
losses and voltage drops due to the lower conductor
with
[1].
resistance, are smaller. Consequently and economically,
Important relationships in connection with power
a smaller cross-sectional area of the transmission line,
consequent
reduced
voltage
drops(IR)
150 L. C. EKECHUKWU, T. C. MADUEME
INTERNATIONAL CONFERENCE ON ELECTRIC POWER ENGINEERING (ICEPENG 2015) OCTOBER 14-16, 2015
with lesser quantity of materials involved in its production, has substantial economic advantage. This
Conductor s
permits the use of thinner conductors. Transmission at higher voltages advantageously result in lower line voltage drop and heat losses (I2R),but renders the high voltage (HV) lines environmentally unsafe to living organisms, making the systems susceptible to ground
Insulators
faults. While research works on conducting materials have been aimed at delivery of electricity at costeffective
and
minimal
ohmic
losses
of
high
Silver Copper Aluminium Iron Carbon(grani te) Water(sea) Water(fresh) Water(distilled) Porcelain Glass Air SF6
y, (ϭ) S/m 6.17x107 5.8x107 3.82x107 1.03x107 1.0x107
ty,ϵr -
4
80 6 5 1.0006 1
10-3 2.10-4 10-10 10-10 -
conductivities but zero permittivity as shown in Table
Source [1]
2,the emergence and applications of non-conducting
II. THE BASIC ENGINEERING CONCEPT AND
materials of very low conductivity and high permittivity
REQUIREMENTS
in power systems have been speedily undergoing several
ENGINEERING PRACTICE.
investigations, also, for higher quality classes of
A. High Voltage Classifications
insulations and dielectrics. This is expedient for the safe-
The IEC definition [2] of high voltage circuits are those
handling of high and extra-high system line voltages.
at applied potentials of more than 1000 V AC and at least
Emerged challenges in transmitting stepped-up voltages
1500V DC. In AC Transmissions high voltage is
along overhead power lines and high voltage system
considered at value range of 35kV – 220kV; extra high
elements, their effects and that of environment (e. g.
voltage (EHV) ≥ 330kV and ˂ 1000kV while ultra high
humidity, rains, lightning strokes, dusts and other
voltage (UHV) levels are 1000kV and above. HVDC
pollutions)on all associated dielectrics and insulations,
levels are below 600kV while UHVDC is above 600kV.
FOR
HIGH
VOLTAGE
necessitated dynamic research and development, leading to the discipline of High Voltage Engineering. Simply put, High voltage engineering practice embraces the study of dielectrics, their characteristics, tests and maintenance, applications to and performance in an integrated
grid.
The
practice
of
High
voltage
engineering, therefore, scopes through types and classes of insulations and their correct applications and behaviours for respective designed and rated generating, transmitting
and
appropriating
relevant
insulations for operations.
High
distributing tests
on
equipment: their
and
associated
safe, efficient and reliable grid voltage
testing
remains
an
indispensable culture in h.v. engineering practice for a reliable grid performance. Table 2 shows properties of
B. Design & Operational Characteristics of Dielectrics for Reliable Grid Performance High Voltage engineering studies basically lie in the fundamental design, concept and roles of the simple capacitor and capacitance phenomenon of a two opposite-facing charged conducting materials (plates or electrodes) separated by a non conducting material called the dielectric (Fig 2). In an operating circuit, the stressed dielectric, usually in the form of gas (e.g. air, Sulphur hexafluoride SF6) or solid (e.g. paper, wood, porcelain, mica, glass, etc) or liquid (e.g. wax, transformer, mineral or vegetable oil, etc), separates the two energised conducting plates facing each other. At a gradual increase of the applied voltage, the ‘sandwiched’ dielectric allows minute leaks of current, called leakage
some conductors and insulating materials.
currents, due to the material’s inherent impurities and Table 2 Properties of Insulating Materials Material
Some
Conductors
Conductivit
and
Permittivit
electrostatic character of capacitors: good dielectrics however disallows flow of high currents across it, till a
threshold voltage is attained across the plate, at which L. C. EKECHUKWU, T. C. MADUEME
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INTERNATIONAL CONFERENCE ON ELECTRIC POWER ENGINEERING (ICEPENG 2015) OCTOBER 14-16, 2015
the dielectric breaks down to conduct electricity. At this juncture the applied potential drives appreciable current through the dielectric. The voltage value at which the dielectric snaps into becoming a conductor is known as the breakdown voltage(BDV) of the particular dielectric and is a function of: (1) purity (quality) of the dielectric, (2)shape of the opposite-facing conducting plates, otherwise known as the electrodes, which is usually of disc, spherical and mushroom designs (Fig 1a) for HV test equipments. (3) the texture of the dielectric determined by its permittivity, (4) thickness of dielectric or distance D, between the plates (Fig 2a) and (5) environmental factors. Absolute perfect dielectric is considered to have zero leakage (capacitance) current, which is practically impossible due to manufacturing processes and material characteristics. Thus, under voltage stress, all dielectrics depending on their degree of purity have the tendency of passing through them, milli/micro/nano values of currents, called leakage capacitance, conduction and absorption currents, whose measured values depend on the prevailing voltage. These currents, under the prevailing voltage stress, give rise to the four respective resistances that total to what is known as the insulation resistance.
It is evident that in the operating power system network connections, short or long line transmission capacitances are introduced by phase-to-phase and phase-to-ground transmission lines. Air serves as their dielectric while the
Fig. 1 High voltage (a) testing vessel for liquid dielectric (b) simplified test circuit for liquid & solid dielectrics
(a) Oil Testing Vessel AVO Foster OTS60 With Mushroom-Type electrodes for Liquid DielectricBreakdown Voltage (BDV) Test. (Courtesy of Ajaokuta Steel Company Limited Ajaokuta) (b)Simplified circuit diagram
conducting lines and ground serve as the plates. In transformers and motors, the windings on one hand and the earthed machines’ bodies on the other hand are the electrodes,
while
conductors’
insulations,
the
impregnated papers, wedges, woods and oils serve as dielectrics. At high voltage (HV) injection test, insulation resistance test and/or any other non- destructive tests, the test equipment outputs are connected at any two convenient points considered as the electrodes for the tested material or specimen.
a)
Simple Capacitor
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dielectrics such as HV transformer bushings, instrument
transformers,
power
cable
insulations, transformer oils and other solid dielectrics like mica, glass, porcelain, etc. A relatively pure capacitor has current leading, by almost 90o, the applied voltage. Presence of
+
+
─
V
impurities like water provides path for resistive components of leakage current in dielectrics which is in phase with the operating voltage across the dielectric. The magnitude of the
─
resistive current tends to zero as the dielectric (b) Simplified circuit diagram Fig. 2
impurity tends to zero thus crediting the
Charged Parallel Arranged Plates
Showing Lines of Electrostatic Forces C. Significance of parameteric tests & measurements for the evaluation of quality status of dielectrics for the enhancement of grid performance
capacitive current maximum and 90O leading the applied voltage. Since no insulator is absolutely pure, a defining ratio-relationship between the magnitudes of the resistive and capacitive components of the resultant leakage currents is required for appraisal of degree of
Tremendous roles are played by insulators in the entire
quality of dielectrics. The resultant leakage
energised grid network, vis a vis:i) security of equipment
current IL lags the vertical y-axis capacitance
from damages at transients - like voltage surges. (ii)
current component, IC, by an angle delta (δ),
security of operating and straying personnel and
called the ‘loss angle’, whose magnitude
mammals from accidental contact with isolated and un-
depends on the purity of the dielectric material,
insulated equipment of the grid. Consequently and as a
while it leads the horizontal x-axis resistance
matter of priority in grids’ safety and reliable operation,
current component, IR, by angle theta (Ѳ),
vital high voltage tests are recommended on associated
known as the power factor angle, as seen in Fig
dielectrics of all power system elements of the grid. This should guarantee reliability and efficiency in grid
3. This appraising ratio-relationship
is
performance. The most vital tests amongst others are: (1)
known as tan δ or tan ‘loss angle’ of the
Tangent (Loss angle) Delta, δ and Power Factor (2)
dielectric. Thus, tan δ =
Insulation Resistance Measurements (3) Breakdown
as IR → 0. Tan δ measurements of grid element
Voltage Tests (4) Leakage Current Measurement (5) Polarisation Index Measurements.
dielectrics therefore remain a very important practice in high voltage engineering (HVE) practice, for assessing the purity and quality of
a) Dielectric Tests •
and is equal to zero
Tangent (Loss Angle) δ Tests, Power &
dielectrics for a continuity or fresh application to the grid. Tangent δ, Dissipation and Power
Dissipation Factor Tests. This is an HV non-destructive test of insulation materials. It is mathematically modelled from the capacitance theory of the capacitor, in determining the tangent δ (loss angle), power factor and dissipation factor measurement of
Factor tests of a dielectric inform of its degree of purity and quality, for application or continuity of usage, in the grid. It is expedient to note that tan δ measurement should be carried out at the normal operating frequency of the grid,
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INTERNATIONAL CONFERENCE ON ELECTRIC POWER ENGINEERING (ICEPENG 2015) OCTOBER 14-16, 2015
so as to give the actual leakage current through the tested
say HV bushing of a 132kV (or more)power transformer,
dielectric when in service. Since frequency determines
in a way that corresponds to the way the specimen is
and is inversely proportional to the magnitude of
usually connected and energised in normal circuit, till the
capacitive reactance of dielectric (
bridge balances. In the case of a current transformer, the
), very
high frequency will make the capacitive reactance very low, resulting in quite high leakage current measurement, and conversely, lower leakage current value than actual at testing with lower frequency than the grid’s normal value of 50Hz as is in Nigeria.
secondary winding and core, connected together, would form the lower terminal of Rx/Cx in Fig. 4b, while the primary winding would be connected to the high voltage terminal of the bridge. Although the usual model for an insulating material (dielectric) is a parallel RC circuit, it is possible to derive an equivalent series RC circuit (Rx and Cx in Fig. 4b).
I=Charging current Current
I
c
I
VAR=I.V.Sin θ
L
δ θ
V=Voltage
W=I.V.Cosθ Fig. 3 Power Factor, Loss angle and Dissipation Factor
(a)
IL = Leakage current IC = Capacitive current = Resistive current
•
I
R
Measurement of tanδ and capacitance with the Schering Bridge The non-destructive measurement of tan δ of dielectric specimen of equipment, such as high voltage bushings of transformers provides information on quality status of
(b)
the insulation. The capacitance and tan δ of insulators is measured by high voltage test equipment called the
Fig, 4 A typical h.v. bushing & basic schematic
Schering bridge, through simultaneous adjustment of
Schering circuit for tangent delta tests
equipments variables and application of test voltage of about 10kV,at the operating frequency, to the specimen,
•
Breakdown Voltage BDV (Destructive) Tests and Leakage Current Measurements
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This test, though seldom used, is considered destructive
lattice arrangements of molecules and insulation bonding
during the test period, for the fact that the dielectric is
while at rest, thus offering least resistance to any current
subjected to almost 200% higher than the normal
flow through the dielectric. At voltage application, with
operating designed values, at which duration the lattice
time, these molecules polarise to form high resistance to
bonding
temporary
further flow of current. The ratio of measured resistance
disorientation. Apart from effect of the presence of
at 600 seconds (10 minutes) R10 to measured resistance at
impurities in dielectrics, fluctuations in voltage stresses
60 seconds (1 minute) R1, i. e. R10/R1 is known as
due to transients and extreme environmental temperature
Polarisation Index (PI). How rapidly this happens tells us
changes and weather conditions also ‘restructure’ the
about the quality condition of the specimen. Capacitance
lattice arrangement of dielectrics, with time, and with a
current affects the first few seconds of PI test;
consequential effects on its quality. Consequently, high
Conduction current should be essentially zero if the
voltage injection tests are carried out on the dielectric at
windings are dry; leakage current is constant over time
very long frequency intervals, to ascertain its fitness for
while absorption current indicates the health of the
continuity on the grid. The test is specifically meant to
insulation. PI measures insulation resistance between the
expose any weak spot of a long serving insulation or
conductor and ground, making it mandatory for the test
further widens an already unidentified ruptured spots of
to be carried out on entirely insulated windings of motors
the insulation. The HV injection values are based on (i)
and/or any other machines, for the avoidance of skewed
how long the dielectric has been in service,(ii) grid’s
(false) result values due to winding parts exposed to
operational history or immediate reason for the test and
vicinity air dielectrics. Accepted dielectric PI ratios [3]
(iii) the provided norms for the test. The idea is that by a
ranges between 2 and 5 as values ˂ 2 suggest dirty or
gradual increase, the applied voltage attains the rupturing
moist winding and values ˃ 5 suggest very dry, brittle
or momentary ‘destruction’ value of the dielectric to
insulation. High voltage pressed-coil insulation (VPI)
conduct. The recorded value becomes the BDV or
systems are exception with PI values between 1 and 2,
‘worth’ value of the material against future transient
considered as perfect good windings. Newer epoxy
over-voltages. Fig 1b is a basic schematic diagram of a
insulation systems have fast reaction time with an almost
specimen subjected to a high voltage breakdown test.
instant polarisation of molecules, such that the PI is
•
structure
is
subjected
to
Insulation Resistance and Polarisation Index
perfectly, almost unity. It should be noted that an energised winding by Megger, Hipot or in service
Measurements. This measurement is a non destructive test usually
operation already has the insulations polarised and will
carried out on power system specimens such as power
certainly offer wrong PI if measured immediately after
cables, circuit breakers, transformer bushings and
shut down. Because it takes time for the molecules to
windings, generators and motor windings, bus bars,
assume their ‘at rest’ positions, it is always advised that
reactors, etc. Insulation resistance values are affected,
the windings must be de-energised long enough to return
most times, by variables such as [3], (1) type of
to rest before commencing PI measurements. Else the
insulation (2) age of the material (3) surface area and (4)
dielectric will take lesser time to polarise, rendering false
environmental factors like moisture and contaminations
PI values.
(dusts).
The
ratio
of
the
applied
voltage
and
any/combination of capacitance, conduction, leakage and
III. METHODOLOGY
absorption generated currents totals to the insulation
Tan (loss angle) δ Test of Bushings of 132/11 kV,
resistance value of the tested specimen. Dielectrics are
63MVA Transformer by Schering Bridge method[4] was
characterised by random orientation and haphazard
carried out at higher oil temperature. Thus the
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INTERNATIONAL CONFERENCE ON ELECTRIC POWER ENGINEERING (ICEPENG 2015) OCTOBER 14-16, 2015
transformer is heated by the no-load magnetising current
capacitance CD-P and tan δ taken, using the Schering
with the automatic cooling system demobilised to
bridge instrument. The entire bushing assembly is held in
prevent automatic cut-in of cooling fans. Thus, Oil Temp
position by the flange, firmly bolted to the earthed
o
at High Side, Th side = 44 C; Ambient Air Temp Tamb =
transformer body. Connections are made between D and
34.5oCAverage Oil Temp, Tave =
F. Capacitance CP-F, between the last metallic band
o
C.
(electrode) P and earthed flange F, is taken during
The vertical bushing input bar, D shown in Fig. 4a has
measurement.
several sheets of oil-impregnated paper wound around it.
Cx
is
obtained
; where
from
the
is the value of chosen
Each layer is separated and held in position by a
formula
cylindrical metallic sheet. The alternating arranged
standard capacitor for the test and is equal to 49.91pf;
cylindrical papers and metal sheets are bound in
is a constant resistor equal to 3183 ῼ;
diminishing area sizes down till the last metallic band,
obtainedfrom the bridge measuring device P5023 of
accessed through the test tap point P. Connections are
former soviet make. At zero balance of galvanometer, G,
made between D and P, and measurement of series
all indicated resistance values are summed up to give
is
A. Manufacturer’s Recommended Test Values Table 3 shows the manufacturer’s specifications of bushing oil when tested at 34 degrees centigrade. Table 3. Temperature of Bushing Oil at Tests = 34OC Tested Phase of Bushing/Plan t No. A (R)
Bushing
Test
Calculated
Measured
Terminal
Voltage
Capacitance,
tgδ of HV Bushing, in
limits of HV Bushing, in
tested
(kV)
(pf)
%, & Angular Degrees
%, & Angular Degrees
D–P
35
C1=342
(calculated)
0
0.56; (0.0097 )
tgδ
Remarks
˂1.2; (0.020)
satisfactory satisfactory
T322
P–F
5
C3=420
1.0; (0.01 )
˂3; (0.050)
B (Y)
D–P
35
C1=325
0.47; (0.0080)
˂1.2; ((0.020))
satisfactory
D88453
P–F
5
C3=460
0.9; 0.0010)
˂3; (0.050)
satisfactory
C(B)
D–P
35
C1=348
0.41; (0.0070)
˂1.2; ((0.020))
satisfactory
79540
P–F
5
C3=410
0
Manufacturers
0
0
˂3; (0.05 )
1.0; (0.01 )
satisfactory
D= Bushing input bar (1st electrode); P=Extreme metal sheet (2nd electrode), F=Earthed Flange; R3 = R1+R2; CX=C1 or C3; C1=Measured capacitance across D-P terminals (1st & 2nd electrodes); C3=Measured capacitance across P-F terminals (2nd & 3rd electrodes)
IV. TEST RESULTS The results of the tests carried out on a 63 MVA, 132/11kV power transformer bushing are shown in table 4 and table 5 respectively. Table 4 Tests Results on operating bushings of 132/11kv, 63 MVA power transformer of Ajaokuta Steel Company(Manufactured In Former Soviet Union); Temperature of Bushing Oil is 39OC. Tested Phase Bushing/Pl ant No.
Insulation
Tested
Test
Calculated
Measured tgδ of HV
Manufacturer’s
Resistance
Specimen
limits of HV Bushing,
Voltag
Capacitance
Bushing,
Across
e,
,
Angular Degrees
P-E(Mῼ)
(kV)
(pf)
A (R) T322
D–P 3000
B (Y) D88453
3000
C(B) 79540
3000
10
C1=357.2
in
%,
&
in
tgδ
Remarks
%, & Angular
Degrees 0
0.745; (0.013 ) 0
P–F
5
C3=524.5
2.34; (0.04 )
D–P
10
C1=336.6
0.549; (0.00950) 0
˂1.2; (0.020)
satisfactory
˂3; (0.050)
satisfactory
˂1.2; ((0.020))
satisfactory satisfactory
P–F
5
C3=559.3
1.245; (0.021 )
˂3; (0.050)
D–P
10
C1=363.4
2.4; (0.0420)
˂1.2; ((0.020))
non-satisfactory
P–F
5
C3=558.6
6.8; (0.1190)
˂3; (0.050)
non-satisfactory
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INTERNATIONAL CONFERENCE ON ELECTRIC POWER ENGINEERING (ICEPENG 2015) OCTOBER 14-16, 2015
D= Bushing input bar (1st electrode); P=Extreme metal sheet (2nd electrode), F=Earthed Flange; R3 R1+R2; CX=C1 or C3; C1=Measured capacitance across D-P terminals (1st & 2nd electrodes); C3=Measured capacitance across P-F terminals (2nd & 3rd electrodes)
Table 5. Repeated test (5 days later) on ht bushings of 132/11kV, 63MVA power transformer after replacement of phase c bushing of previous poor tan δ readings. Temperature of Bushing Oil ts 37OC. Tested Phase Insulation Bushing/Plant Resistance No. Across
Tested
Test
Calculated
Measured tgt δ
Manufac
Specimen
Voltage,
Capacitance,
&
turer’s
(kV)
(pf)
Angular Degrees
Remarks
tgt δ limits
P-E
&Angular
before
Degrees
HV injection (Mῼ) A (R)
3000
T322 B(Y)
P–F 3000
D88453 C(B)
D–P
3000
10 5
C1=355.4 C3=529
0.525; (0.0090) 0
1.50; (0.026 ) 0
˂1.2; (0.020) 0
˂3; (0.05 )
satisfactory satisfactory
0
D–P
10
C1=336.64
0.525; (0.009 )
˂1.2; ((0.02 ))
satisfactory
P–F
5
C3=570.63
1.0; (0.0170)
˂3; (0.050)
satisfactory
D-P
10
C1=359.88
0.48; (0.0080)-Replaced ˂1.2; ((0.020))
79537
satisfactory
bushing P-F
5
C3=507.58
0.98; (0.0170)-Replaced ˂3; (0.050)
satisfactory
bushing
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D= Bushing input bar (1st electrode); P=Extreme metal sheet (2nd electrode), F=Earthed Flange; R3 R1+R2; CX=C1 or C3; C1=Measured capacitance across D-P terminals (1st& 2ndelectrodes); C3=Measured capacitance across P-F terminals (2nd & 3rd electrodes)
•
C
–
phase
bushing
dielectric
was
recommended for replacement; was effected and tested for tangent delta, with test values of0.48; (0.0080) and
V. ANALYSIS OF TEST RESULTS
0.98; (0.0170), as shown in Table 5,
The results of tangent delta tests informing the
measured across D – P and P – F
status of HV bushings of the three phases of a
electrode
typical 132/11kV, 63 MVA transmission power
These test values are almost as
transformer have been presented. As the power
qualitative
transformer is a vital power equipment that
factory and pre-operational values as
enhances efficient grid performance the following
shown in table 3.
findings and
measures to
forestall possible
•
transformer breakdown and system collapse are
The
manufacturing
manufacturer’s
Most of the obtained loss angle values are
and
demonstrating high level of purity
commissioning (1982) value for the
expected of bushing dielectrics for
tangent delta test of C-phase HT
grid
bushing, measured across terminal
transmission transformers.
in Fig. 4a, was 0.41; (0.0070) and 1.0; (0.010) respectively as shown in Table 3,was
quite
satisfactory
conforming
to
and
manufacturer’s
standard. By
the
as seen in Tables 3, 4, 5, thus
factory’s
electrodes D – P and P – F as shown
•
as
respectively.
within 1st and 2nd decimal zero ranges
hereby highlighted: •
terminals
June
•
network elements,
Deterioration
few
years
of
grid
as
dielectrics
is
unnoticeably gradual and could be misleading observations qualities operational
1988,
of
such
ascertained
if
judged only.
and
by
visual
Hence
their
suitability
for
continuity
must
be
through periodic
non
commissioning and operation of the
destructive and at seldom, high
transmission transformer, the tan δ
voltage injection tests.
value of C-phase bushing was tested and found deteriorated, while A & B
VI. CONCLUSION
phases tested qualitatively satisfactory
This paper has highlighted the importance, types of
as shown in Table 4. The tangent
dielectrics in high voltage networks and the tests
delta readings across electrodes D – P
that are performed to ensure reliability of the power
and P- F of C – phase bushing, was
grid. In this work it has also been ascertained that
found to be 2.4; (0.0420) and 6.8;
system equipment should be guided by high
(0.1190)
signifying
voltage practices, including subjection to high
highdifferentialsby1.2;
voltage tests of their dielectrics, so as to promptly
3.8 (0.069O) above
zero down delays in the identification, speed and
manufacturer’s limits of 1.2; ((0.02)
quantity, of deteriorating insulations, in the interest
and 3; (0.050) respectively.
of safety of equipment, personnel, reliability and
respectively,
substantial ((0.0220)) and
integrity of the integrated network as a whole. Test
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INTERNATIONAL CONFERENCE ON ELECTRIC POWER ENGINEERING (ICEPENG 2015) OCTOBER 14-16, 2015
results on a 63 MVA power transformer bushing oil has been presented and analyzed. It is certain that high voltage engineering practice will remain a sine qua non, in decades to come, a vehicle for the enhancement of national grid performance, as more research findings and innovations for further improvement of dielectric qualities are made public.
REFERENCES. 1
Holtzhausen J. P, Vosloo W. L. ‘High Voltage Engineering Practice and Theory’ Electrical Engineering Portals, https://app.box.com/s/x7froiv7q2lzpocbgh35, 2015
2
Jian L. I. ‘Introduction to Fundamentals of High Voltage Engineering’, Department of High
Voltage & Insulation Engineering,
Chongqing
University.
www.cee.cqu.edu.cn/myweb/upfile/200903091 45343432.pdf, March 9, 2009
3
Yung
Chuck,
EASA
Technical
Support
Specialist. ‘Use Polarisation Index Test to Determine
Condition/Health
of
Motor
Insulation’, www.easa.com. September 2000
4
Ajaokuta Steel Company limited Ajaokuta, Kogi State, Nigeria ‘High Voltage Tests & Maintenance Records’ 1988
159 L. C. EKECHUKWU, T. C. MADUEME