1.1 GENERAL
In onshore
installations main electric power is taken in bulk from the National Grid
through Area Boards at voltages up to 33kV.
In offshore installations however main power must be generated locally,
and this is usually done at 6.6kV.
Note that 6.6kV is a nominal
rating; in practice generation is more usually at 6.8kV to allow for voltage
drop in the network.
There are instances of
generation at other levels, but these are always ‘high voltages’. Some large loads are fed directly from the HV
system, but for most purposes the supplies are needed at low voltage, typically
440/250V offshore and 415/240V onshore.
These are provided through 3-phase power transformers.
FIGURE 1.1
THREE PHASE OIL FILLED
TRANSFORMER
1.2 CONSTRUCTION
Power transformers are
always enclosed in a tank or similar protection. They may be liquid cooled, air cooled or dry
type (encapsulated or open). If liquid
cooled, the coolant may be mineral (hydrocarbon) oil, silicone oil or some
artificial liquid such as ‘Askarel’.
The internal
construction of all power transformers is similar. The windings are stacked around a 3-limbed
laminated iron magnetic core, the low-voltage windings innermost and the
high-voltage windings outside them - the best arrangement for insulation. It can be seen in the cut-away portion of
Figure 1.1. Ducts are arranged through
both windings on each limb to assist cooling.
The terminations of the windings are brought out to cable boxes for
external connections (see para. 1.8) or, for large outdoor transformers, to
terminal bushings.
The largest bulk-power
transformers are usually in a single tank, completely filled with oil and with
a header tank called a ‘conservator’ on the roof. This maintains a static head of pressure on
the oil and also allows free expansion and contraction. The transformer of Figure 1.1 is of this
type.
In the pipe connecting
the main tank to the conservator there is often inserted a device called a
‘Buchholz Relay’. It has two elements:
one traps and collects any small gas bubbles evolved at a winding due to the early
stages of a possible breakdown of insulation.
If sufficient gas has accumulated, a float switch gives an alarm. The other element is a pivoted vane. If a major fault occurs inside the tank, the
displaced oil surges past the vane, causing it to swing, make a contact and
trip the supply breaker. The Buchholz
relay is further described in the manual ‘Electrical Control Devices’.
The oil coolant is
heated by the I2R losses of the currents in all the windings
and also by the iron losses. It circulates through a closed cooling system by
thermosyphon action (in a few cases by pumping). Heat is extracted from the coolant through
radiating tubes or fins either by natural convection, by forced cooling from
fans or, more rarely, by water cooling.
The cooling of transformers is dealt with more fully in para. 1.6. The whole arrangement can be seen in Figure
1.1.
Facilities are
provided for oil filling, draining and sampling for test. Oil samples are taken periodically for
insulation testing in the laboratory, where they are examined for deterioration
or water pollution.
A tapping switch,
normally for off-load use only, is usually fitted for changing the transformer
taps. The larger system network transformers may have on-load tap-changing gear
- see para. 1.9 for details.
Smaller oil-filled
transformers are usually sealed, with an air space above the oil instead of a
conservator, to allow expansion when hot.
In appearance they would look like the Askarel-filled type shown in
Figure 1.2.
Silicone oil is increasingly
used instead of mineral oil because it is non-flammable. The construction is however similar.
In onshore
installations where transformers can be installed at a distance from other
plant, the fire risk is no greater than normal, and mineral oil-filled
transformers are generally used.
Offshore however the fire risk is crucial, and other designs of
transformer are necessary.
For this reason power
transformers on offshore installations do not use mineral oil as the insulating
and cooling medium. Instead, a
non-flammable silicone oil or a non-flammable liquid such as Askarel is used
which is sometimes described by a trade name such as ‘Pyroclor’ or ‘Pyralene’.
The basic transformer
design using silicone instead of mineral oil is no different from that
described for oil-filled transformers.
But Askarel, apart from its fire-resistant properties, has other
characteristics, namely:
·
it is expensive,
·
it evaporates readily when in contact with air,
·
it is very penetrating,
·
it is heavy,
·
it is toxic and must not be allowed to come into contact with the skin
or eyes,
·
it must on no account be discharged into the sea because it is
non-biodegradable.
The external
appearance of a typical Askarel-filled transformer is shown in Figure 1.2. Its internal construction is as described in
para. 1.2.1, but, additionally, the transformer is hermetically sealed to
prevent loss of liquid by evaporation. In
some designs the main cover flange joint is welded up, as is also the filler
plug after filling with liquid, and sometimes even the drain plug. The expansion space above the liquid is
filled with dry air or inert gas and has sufficient volume to ensure that the
pressure inside the tank is limited to a safe value even at maximum temperature
and expansion. A pressure/vacuum gauge
is fitted. It indicates zero at normal
temperature, a positive pressure at high temperature and a partial vacuum at
low temperature. This gauge is a
constant monitor on the state of the sealing.
A sight-glass also gives a direct measure of the liquid level at all
temperatures.
FIGURE 1.2
TYPICAL 2 000kVA SEALED
POWER TRANSFORMER (ASKAREL FILLED)
The off-load tapping
switch spindle has five positions.
Because Askarel is a penetrating
liquid it is not easy to provide an adequate seal where the operating shaft of
the tapping switch comes through the tank-wall of the transformer. Some designs rely on a simple packing gland
whereas others back this up by enclosing the whole tapping switch handle in an
auxiliary box with a bolted cover. This
box is filled with Askarel and provides a second barrier to prevent liquid from
leaking out of the main tank. With the
latter design it is necessary to drain and open up the auxiliary box to get at
the tapping switch handle.
If a fault develops
inside the transformer, the Askarel breaks down and forms a gas leading to a
gradual or sudden rise in pressure, depending on the severity of the
fault. To prevent the transformer tank
from splitting, a spring-loaded ‘Qualitrol’ pressure relief device on the top
operates to release the excess pressure; at the same time contacts within the
device close to trip the incoming supply and give an alarm. Pressures encountered in normal service are
not high enough to operate the device, which is essentially an emergency relief
valve. The Qualitrol device is further
described in the manual ‘Electrical Control Devices’.
In case the tank
should ever crack or split and so spill the Askarel, these transformers are
always erected with a sill around their mounting places. The sill is high enough to contain the entire
filling of its transformer and to prevent the toxic liquid spreading. After a spill the liquid must be collected
and put into containers, along with mopping-up rags, and sent ashore for
disposal. ON NO ACCOUNT MAY THEY BE
DROPPED INTO THE SEA. Personnel
cleaning up must wear protective clothing, gloves and goggles.
Though widely used
offshore at first, Askarel-filled transformers are gradually being phased out
in favour of silicone oil-filled types because of the toxic nature of Askarel.
On some offshore
installations transformers are used where the windings are encapsulated in
epoxy resin and the whole block is air cooled.
To assist the cooling, air ducts are arranged through the solid
encapsulation.
Such transformers are
often given a dual rating (e.g. 2 000/2 500k VA): the lower one where
the cooling air circulates naturally, and the higher one where it is assisted
by fans. It is arranged that the fans
start automatically when the loading of the transformer exceeds the lower
rating.
Dry-type power
transformers can readily be built into their own LV distribution switchboards
to form a single unit, thereby saving LV cable boxes and cables and bringing
the incoming feeder copperwork right up to the transformer’s LV terminals.
Small low-voltage
transformers used as part of other equipment - for example, in battery chargers
or inverters - are usually open type, air cooled without any enclosure. They may be 3-phase or single-phase. Such open-type transformers are protected by
being housed within the parent equipment’s main enclosure.
1.3 RATINGS
The capacity of
transformers is always given in kVA or MVA, because the heating depends only on
the actual current and is not affected by the power factor of that current.
The ratings of most
offshore power transformers extend over a range of about 400kVA to
2 500kVA, depending on their duty. In onshore installations the ratings may go up to 30MVA or more; National Grid sizes may go up to 750MVA.
2 500kVA, depending on their duty. In onshore installations the ratings may go up to 30MVA or more; National Grid sizes may go up to 750MVA.
A transformer is
designed to give a nominal secondary voltage from a nominal primary voltage -
for example 11 000/415V or 6 600/440V. Due to voltage drop within the transformer
itself, the actual turns ratio must be somewhat lower than this if the nominal
secondary voltage is still to be achieved at full load. In the two examples cited above the turns
ratio (that is, the no-load ratio) would need to be about 11 000/435V and
6 600/460V respectively.
Alone among electrical
plant, transformers are required by British Standards to have their no-load
rating displayed on their nameplates (generators and motors have their
full-load ratings). The nameplate figure
is therefore sometimes misleading in that it suggests a 435V or 460V system,
whereas the nominal system voltage is still 415V or 440V. In some documentation only nominal
voltages are normally used, notwithstanding any transformer name-plate
figures. Errors due to this
misunderstanding may often be found on other drawings.
1.4 IMPEDANCE VOLTAGE AND REGULATION
In a manner similar to
generators, transformers present impedance to the flow of
through-currents. This impedance is
measured by the percentage voltage applied at rated frequency to the primary
winding necessary to circulate full rated current in the secondary when
short-circuited.
The effect of
transformer impedance is to cause an internal voltage drop when load current is
passed through the transformer. Exactly
as with a generator, the greatest drop is caused when a reactive current passes
through the reactance of the transformer. (The vectorial treatment of impedance loading
on a generator is fully covered in the manual ‘Electrical Generation
Equipment’, Chapter 4.)
The internal drop due
to load current causes a reduction of the secondary terminal voltage below its
open-circuit level. This reduction,
usually expressed as a percentage of the no-load voltage, is termed the
‘regulation’ of the transformer under the stated load conditions. Since the impedance of a transformer is
almost wholly reactive, it follows that the greatest regulation occurs when a
highly reactive load is applied.
If E is the nominal rated line voltage
applied to the primary winding, and if Esc is the line
voltage which, when applied to the primary, will circulate full rated current
in the short-circuited secondary, then
Z |
=
|
Esc
|
E
|
Esc is called the ‘impedance voltage’ of the transformer and is usually
expressed as a percentage of E. This same percentage gives the value of Z, which is the
‘percentage impedance of the transformer’.
This impedance is
almost pure inductive reactance and ranges in value from about 5% to 10% for
the sizes of transformers in use. The
measured percentage impedance is marked on each transformer nameplate and is
used, together with other circuit impedances, to calculate the symmetrical
short-circuit level on the low-voltage system. (See the manual ‘Electrical
Protection’.)
At the instant of
switching on a transformer, while the core is unfluxed and therefore offers no
reactance, a large ‘inrush current’ will flow which, although transient, may
achieve a value of up to five times full-load primary current. This disappears quickly after switch-on.
Once the core is
magnetised, the impedance of a transformer to fault currents is constant; this
contrasts with a generator whose reactance changes from subtransient through
transient to synchronous as a fault progresses.
1.5 INSULATION
The maximum
temperature to which the windings of dry-type transformers may be allowed to
rise depends on the type of insulating material round the conductors. These
transformers are classified according to the insulating material used, and to
each class is allotted a maximum ultimate temperature. The classification is as
follows (according to BS 171 : 1970 and BS 2757 : 1956):
Class
|
Typical Insulating Material
|
Ultimate Temperature
|
A
|
Impregnated cotton,
silk, etc.; paper; enamel
|
105oC
|
E
|
Paper laminates;
epoxies
|
1200C
|
B
|
Glass fibre, asbestos
(unimpregnated); mica
|
130oC
|
F
|
Glass fibre,
asbestos, epoxy impregnated
|
155oC
|
H
|
Glass fibre,
asbestos, silicone impregnated
|
180oC
|
C
|
Mica, ceramics,
glass, with inorganic binders
|
> 180oC
|
It should be noted
that the classification letters do not follow an alphabetical sequence. This is because there were originally only
three classes - ‘A’, ‘B’ and ‘C’. Later
intermediate classes were added, and it was decided not to disturb the original
well-understood three.
Certain of the
higher-temperature materials may be hygroscopic and therefore not always
suitable in any particular environment, particularly where dampness is severe.
It should be
particularly noted that the classification depends on the ultimate
temperature to which the insulating material may be subjected, for it is this
which determines whether or not it will suffer damage when heated. It does not depend on temperature rise
alone. If, for instance, the ambient
temperature is 40oC, a Class ‘B’ material may be used if the
designed temperature rise will not exceed 90oC, so making the
ultimate maximum temperature 130oC.
Designed temperature rises must therefore take into account the greatest
expected ambient temperature in which the transformer will operate.
Liquid-filled
transformers are not classified for insulation as are the dry type. There is an overall requirement that the
temperature rise of the windings shall not exceed 65oC, and
that the temperature rise at the top of the liquid shall not exceed 60oC
if the transformer is sealed or has a conservator.
1.6 COOLING
The cooling system of
a given transformer is identified by a 4-letter code, as follows:
1st
and 3rd letter: kind of cooling
medium
2nd
and 4th letter: kind of
circulation
The code symbols for
the first and third letters are:
Mineral
oil O
Synthetic
insulating liquid L
Gas G
Water W
Air A
Solid
insulant S
The code symbols for
the second and fourth letters are:
Natural
circulation N
Forced
circulation F
Examples of the use of
this code are:
Oil-filled,
thermosyphon circulation, natural ventilation ONAN
Askarel-filled,
thermosyphon circulation, natural ventilation LNAN
Dry-type
encapsulated, fan cooled SNAF
Oil-filled,
pumped circulation, water cooled by pump OFWF
1.7 THREE PHASE TRANSFORMER CONNECTIONS
A 3-phase transformer
has a 3-limb core. For transformers designed to BS 171 the terminals of
the windings mounted on each limb are identified by a letter as shown in
Table 1 overleaf.
Table 1 overleaf.
FIGURE 1.3
WINDING AND TERMINAL MARKINGS
TABLE 1. DESIGNATING LETTERS FOR
3-PHASE TRANSFORMERS
Winding
|
Designating Letter
|
||
Limb 1
|
Limb 2
|
Limb 3
|
|
High Voltage
|
A
|
B
|
C
|
Low Voltage
|
a
|
b
|
c
|
Tertiary (if fitted)
|
3A
|
3B
|
3C
|
The external
connections to the high- and low-voltage windings are brought out of the tank
through bushings. These terminals are labelled using letters
appropriate to the winding concerned as shown in Figure 1.3. When viewed from a position facing the
high-voltage side of the transformer, the phase sequence is A-B-C from left to
right. The subscript numbers identify
the winding terminations, including tappings, numbered in the direction of the
applied or induced voltage at a given instant.
Three-phase windings
can be connected in delta, star or zig-zag (not very common); the star or
zig-zag connection must be chosen if a star-point is required to provide a
neutral for a 4-wire system or for earthing.
A common arrangement for 3-phase power transformers in both onshore and
offshore installations is for delta-connected high-voltage windings and
star-connected low-voltage windings, with the star-point brought out to provide
a neutral and earth for the low-voltage system.
A delta-connected
winding is designated by the letter ‘D’, a star-connected winding by ‘Y’ and a
zig-zag winding by ‘Z’. Capital letters
are used for the high-voltage windings and lowercase for the low-voltage. Thus ‘Dy’ stands for delta HV/star LV; Yy for star HV/star LV, and so on. When the star-point of a star-connected
winding is brought out it is designated ‘YN’ for a high-voltage or ‘yn’ for a
low-voltage winding.
The winding
connections for a delta/star transformer having a delta-connected high-voltage
winding are shown in Figure 1.4, which also shows the vector relationship
between the voltage applied to each high-voltage winding and the induced
voltage in each corresponding low-voltage winding, the reversal between
secondary and primary being ignored.
Taking the phase-to-neutral
vector of ‘A’ phase high-voltage as reference vector at
12 o’clock, the corresponding ‘a’ phase low-voltage vector leads by 30o and is therefore at 11 o’clock. Thus the vector symbol in this particular connection arrangement is ‘Dy11’, which describes the high- and low-voltage winding connections and the angular displacement between primary and secondary voltages. Other winding arrangements are sometimes used, and for full particulars of these, together with their vector symbols, reference should be made to BS 171 - Specification for Power Transformers.
12 o’clock, the corresponding ‘a’ phase low-voltage vector leads by 30o and is therefore at 11 o’clock. Thus the vector symbol in this particular connection arrangement is ‘Dy11’, which describes the high- and low-voltage winding connections and the angular displacement between primary and secondary voltages. Other winding arrangements are sometimes used, and for full particulars of these, together with their vector symbols, reference should be made to BS 171 - Specification for Power Transformers.
In the case shown
above the vector symbol is sometimes written ‘Dyn11’ to draw attention to the
neutral’s being brought out on the secondary (low-voltage) side.
Transformers of
different vector groups must not in general be paralleled. If all the primaries are supplied from a
common source, the secondaries of differing groups such as Dy11, Dy1, Yy0 will
have different phase relationships. For
example, there will be 60o difference between Dy1 and Dy11 (which
leads on it), or 30o difference between Yy0 and Dy1 (which lags on
it). Such out-of-phase secondaries must
never be paralleled, even though their primaries may be in parallel.
The exception is that
groups with the same clock numbers, such as Dy11, Yd11, Yz11, may be
paralleled, provided that there is no other objection, since the secondaries
are all in phase.
FIGURE
1.4
VOLTAGE VECTOR SYMBOLS
1.8 CABLE BOXES
The terminals of large
transformers which are connected to external lines are brought out through
ceramic bushings in the cover (shown in Figure 1.1). The terminals of other transformers have to
be connected to cables. This applies
particularly to transformers on offshore installations and to most transformers
in onshore oil installations.
The windings are
connected to cables through cable boxes fixed to the transformer tank. If cables are used on both HV and LV sides, the cable boxes
would be on opposite sides of the tank, as seen in Figure 1.2.
On most transformers
the current on the HV side is low enough to be carried by a single, 3-core cable
which enters the HV box through a sealing gland and divides inside. Sometimes small current transformers are also
fitted inside the cable box.
On the LV side currents are much
heavier and often exceed 3 000A.
The LV
cable box is therefore much larger. In
order to carry such currents, three, or sometimes four, single-core cables are
required for each phase. This results in
the cable runs in the area of a transformer being very heavy and often
difficult to accommodate. In addition
there may be two similar-sized cables to carry the neutral, or 4th-wire,
current.
On some installations
the LV cable
box is dispensed with and the windings are connected directly to the
switchboard by busbar-type copperwork in an enclosed duct which is brought
right up to the side of the transformer.
1.9 TAP CHANGING
Tappings are usually
provided to vary the transformer’s turns ratio by up to ±5%. The
correct tap is set when the installation is first commissioned and should not
need to be changed for a considerable time.
However, as the system load grows over the years, the tapping may need
to be changed to maintain the secondary working voltage. This is normally done on all phases together
by means of a switch on the transformer tank and must only be carried out off-load and isolated -
that is, with the transformer dead on both sides. Changes of tap settings may be carried out
only by Authorised Persons, and then only on the instructions of the
Engineering Department. All tap changers
on offshore and onshore oil installations are of the off-load type.
In the larger shore
networks on-load tap changers may be used to maintain system voltage;
they are usually remotely controlled from a Control Centre and are described in
para. 1.9.3. On-load tap changers are
not used on offshore or onshore oil installations but may be employed on the
networks supplying onshore plants.
It is usual to provide
four additional tappings with off-load tap changers, making a total of five, at
2½% intervals, so that the turns ratio varies by ±2½% ±5%. Tappings
are always placed on the high-voltage side; this allows the lowest possible
current rating for the tapping switch itself.
Thus an 11 000/415V transformer with four such extra tappings would
be shown on a drawing as ’11 000 ±2½% ±5%/415V’ and would actually give 11 000/394, 405, 415, 425 or 436V on load. In order to raise the secondary voltage it is
necessary to go to a lower (i.e. negative) HV tap.
The tap-changer switch
handle can be seen in Figure 1.2. It
must always be kept padlocked against unauthorised or accidental operation.
Large network
transformers which are provided with on-load tap changing normally have a much
larger number of taps in smaller steps. The principle used is ‘make-before-break’:
this means that the new tap must be connected before the old tap is broken,
otherwise there would be a break in supply and an interruption of full-load
current by the tapping switch.
The difficulty with
this simple idea is that, during the transition period while both taps are
made, a small number of turns of the transformer’s HV winding are
short-circuited by the two taps, and a heavy current will flow through
them. Arrangements are therefore made to
insert resistance temporarily into this short-circuited loop to limit the
current until the tap change is complete and the short-circuit removed. Figure
1.5 shows in principle how this is done.
FIGURE 1.5
ON LOAD TAP CHANGING
A, B and C are
adjacent taps on an HV winding. In (a)
the tapping is on A, and it is desired to move it, on load, to B.
The moving member
consists of a main contact M and two ‘transition’ contacts P and Q which are
connected to M each through a resistance.
In position (a) M carries the full load, and P and Q are not in contact.
In the first part (b)
of the transition the main contact M is still on tap A. Contact Q moves to B and contact P is still
on A. Q and M now short-circuit the HV turns between A and B, but the
short-circuit current is limited by the lower half of the resistance. Meanwhile M is still carrying the load
current from tap A.
At the next stage (c)
the moving member has travelled on, and the main contact M leaves tap A. P and
Q now share the load current which passes through both halves of the
resistance. These two halves also limit
the current in the shorted turns between A and B.
At the next stage (d)
the main contact M has moved to tap B, so that it is once again carrying the
load current, but now from the new tap. P
however is still on tap A, so that the current from the shorted turns is
limited by the upper half of the resistance.
Finally the moving
member is at position (e), where the main contact M is on B and carrying the
load, while P and Q are out of contact, as they were in position (a), but now
on the new tap.
During these
transition stages the load current has never been interrupted, nor has the main
contact ever been called upon to break any large current. Moreover the current in the short-circuited
turns is always limited by one or both halves of the resistance.
In some designs of tap
changer the transition resistors are replaced by reactors. These have a similar limiting effect but are
not a source of heat. They also cancel
each other out magnetically in stage (c) when both are sharing the load.
During stage (c) the
full-load current passes momentarily through both halves of the
resistance. To keep them to a reasonable
size, they must be short-rated. This
poses the problem that, if the driving motor power should be lost at the moment
the mechanism reached stage (c), it would stick there and a rapid burnout of
the resistors would follow, with inevitable damage to the short-circuited
turns. Steps must therefore be taken to
prevent this happening.
The philosophy is that the power to
operate the tap-changer mechanism must never do so directly but should be used
only to store energy. When a tap change
is called for, that energy is released and is sufficient to complete the change
on its own, even if the external power supply fails.
The stored-energy
tap-changer mechanism is usually of one of two types - spring-operated or
flywheel-operated. In the former a motor
winds and charges a spring. A tap change
cannot begin until the spring is fully charged, and, once released, it
completes the change on its own.
In the flywheel type a
motor runs up a flywheel on receipt of a tap-change signal. When the wheel is up to full speed the motor
is disconnected and a clutch engages.
The kinetic energy of the flywheel completes the change on its own.
On-load tap changers
and their operating mechanisms are usually separate assemblies bolted to the
transformer tank, through which the tappings from all three phases are brought
out into the changer compartment. This too
is usually oil filled but separate from the main tank, so that the tap changer
can be drained for maintenance without having to drain the main tank.
Provision is made for
manual operation, if that should be necessary, by inserting an operating
handle. The speed of the tap change
remains the same as with power operation, since the same stored energy is
released.
FIGURE 1.6
AUTO TRANSFORMER CONNECTION
1.10 AUTO TRANSFORMERS
Where a transformer
ratio is fairly close - for example 3:1 or less - there is much advantage in
both cost and weight in combining the primary and secondary windings, as in
Figure 1 6(a). Such an arrangement is
called an ‘auto-transformer’.
In Figure 1.6(a) the
secondary winding is combined with the primary, one terminal of each being
common; the other secondary terminal is effectively a tap on the primary
winding. This arrangement gives a
step-down effect, like a potentiometer, depending on the primary/ secondary
turns ratio. Since the primary and
secondary currents are in opposition, the net current in the common part is less
than the secondary current alone. For
example, if the primary current were 100A and the ratio 3:1, the secondary
current would be 300A, and the net current in the common part would then be the
difference, namely 200A. This part of the winding could therefore be
of lighter construction than would be needed if the transformer had been of the
normal double-wound type. Also, because
of the closer linkage between the primary and secondary windings, there is less
leakage reactance, and the reactance of an auto-transformer is in general less
than that of its double-wound counterpart.
Although Figure 1.6(a)
shows a voltage step-down arrangement, an auto-transformer can equally be used
for stepping up (unlike a potentiometer), as in Figure 1.6(b). This is possible because the primary flux
still links the whole of the secondary winding, so developing in it the full
emf determined by the secondary turns.
Use of an auto-transformer is a very economical way of converting, for
example, control supplies from 110V to 220V or vice versa.
Because a double-wound
transformer provides complete electrical isolation between the two sides, an
earth fault on one side is not carried over into the other. This is not the case however with an
auto-transformer. Both sides are
electrically connected through the common terminal and the ‘tap’.
It is important for
reasons of safety that, if one line is earthed on one side, that earth should
be applied to the common terminal so that it is also applied to both sides, as
shown in Figure 1.6(c). In that case, if
the primary voltage were 220V and the secondary 110V, the common earth would
ensure that the ‘live’ secondary terminal would never be more than 110V to
earth.
A safety hazard would
exist if an auto-transformer were wrongly connected, as shown in Figure
1.6(d). Here the earthed line is not the
common one, with the result that there is now no direct earth on the 110V
system, one line being at 110V and the other at 220V to earth - a possibly
dangerous situation when the secondary circuit is switched in one pole only.
This error can easily
arise when domestic equipment which has been designed for the USA 110V system
is adapted to operate from the UK
240V supply. Any such adaptations should
always be carefully checked for polarity.
1.11 TRANSFORMER TESTING
All power transformers
are subjected to extensive tests by the manufacturers before delivery to the
customer. While operators and
maintenance staff are not responsible for carrying out these tests, it is
obviously an advantage to have some knowledge of them. They are summarised overleaf. If more details
are required, reference should be made to BS 171:1970 - Specification for Power
Transformers.
Tests by the
manufacturer are of three kinds:
Routine A
test to which each individual transformer is subjected.
Type A test made on a
transformer which is representative of other transformers, to demonstrate that
they comply with specified requirements not covered by routine tests.
Special A test other than a type
test or a routine test, agreed by the manufacturer and the purchaser, and
applicable only to one or more transformers of a particular contract.
Routine tests
comprise:
(a) Measurement
of winding resistance, using a d.c.
source and taking account of temperature.
(b) Ratio,
polarity and phase relationships, in which the voltage ratio is measured on
each tapping. The polarity of
single-phase transformers and the vector group symbol of 3-phase transformers
are checked.
(c) Impedance
voltage, using an a.c. source at the rated frequency, and carried out between
pairs of windings. Impedance voltage is defined in para. 1.4.
(d) Load losses, at rated frequency and
carried out between pairs of windings.
(e) No-load losses and no-load current,
measured at rated voltage and frequency.
(f) Induced
overvoltage withstand: a test of dielectric insulation using a source of
higher-than-rated frequency to avoid excessive excitation current.
(g) Separate
source voltage withstand: similar to (f) but using a source not less than 80%
of the rated frequency.
(h) The
insulation resistance of each winding in turn to all other windings, core and
frame or tank, all connected together and to earth. (Note: Where windings are star-connected or
delta-connected inside the transformer, phase-to-phase insulation tests cannot
be carried out.)
Type tests and special
tests are made only if specified by the purchaser. They include:
(j) Temperature
rise test.
(k) Impulse-voltage withstand tests (with
and without chopped waves).
(I) Measurement of zero-phase sequence
impedance.
Operators and
maintenance staff, while not responsible for the manufacturers’ tests referred
to above, are required to apply certain routine checks and tests to power
transformers at the intervals laid down in the appropriate maintenance
schedules.
These routine tests
include:
(a) Visual
examination of the transformer and its earthing resistor (if any), cable
connections and earthing arrangements for tightness, mechanical damage,
corrosion and signs of overheating.
(b) Checking the oil or Askarel levels and
inspecting for leaks and clear drains.
(c) High-voltage
insulation resistance test on the HV windings.
(d) Low-voltage
insulation resistance test on the LV
windings.
(e) Simulation of overtemperature and
overpressure by manual operation of the protection devices, and checking that
the alarm indications appear and the circuit-breaker trips.
1.12 TRANSFORMER PROTECTION
The protection of electrical installations,
including transformers, against damage caused by overload or fault conditions
is described in the manual ‘Electrical Protection’. To summarise, the protection provided for
transformers may consist of one or more of the following:
HV Side Overcurrent
Earth fault
LV Side Restricted
earth fault
General Overpressure (‘Qualitrol’)
Overtemperature
Buchholz
(oil-filled only)
Differential
3 comments:
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"MBT is a brand of Electrical Transformer that has a high reputation in the Vietnamese market. Our main products are: Dry-type transformer, oil-immersed transformer, electrical cabinet. Our product is supplied for big project in Cambodia, Laos, Australia,... If you need quotation, please contact me:
Our website:
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