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A
transformer is an electrical device that
transfers energy from one circuit to another
by magnetic coupling with no moving parts.
A transformer comprises two or more coupled
windings, or a single tapped winding and,
in most cases, a magnetic core to concentrate
magnetic flux. A changing current in one
winding creates a time-varying magnetic
flux in the core, which induces a voltage
in the other windings, and usually at a
different voltage as compared to the other
winding.
A
simple transformer consists of two electrical
conductors called the primary winding and
the secondary winding. Energy is coupled
between the windings by the time-varying
magnetic flux that passes through (links)
both primary and secondary windings. Whenever
the amount of current in a coil changes
(including when the current is switched
on or off), a voltage is induced in the
neighboring coil. The effect, called mutual
inductance, is an example of electromagnetic
induction.
Common
Industry Standards
Underwriters
Laboratories Inc. (UL) is an independent,
not-for-profit product safety testing and
certification organization. The following
are classifications of Underwriter Laboratories.
* Transformers, General Purpose (XPTQ.E46323)
The transformers covered by this listing
are of the compound filled, exposed core
or open core and coil construction, (industrial
control type), rated 600 v or less. Step-up,
step-down, insulated, and autotransformer
types as well as air cooled reactors are
included. Autotransformers are so marked.
for more information.
*
Transformers, General Purpose - Component
(XPTQ2.E46323)
This category covers compound filled, exposed
core and open core and coil transformers
rated 600 v or less. Step-up, step-down,
insulated and autotransformer types as well
as air cooled reactors are included in this
category.
*
Power and General Purpose Transformers,
Dry Type - Component (XQNX2.E97674)
These transformers are of the air cooled
dry, ventilated or nonventilated type rated
600 v or less; 500 kVA or less single phase;
and 1500 kVA or less three phase. Step-up,
step-down, insulated and autotransformer
types as well as air cooled reactors are
included.
*
Systems, Electrical Insulation - Component
(OBJY2.E65096)
This category covers combinations of insulating
materials arranged to form an insulation
system such as that used in motors, transformers,
solenoids, etc. Also included are coated
core (integral ground) insulation constructions.
The
CSA Mark (Canadian Standards Association)
signifies that an authorized testing laboratory
has evaluated a sample of the product to
determine that it meets applicable national
standards CSA tests and certifies products
to applicable safety or performance standards
including ANSI, ASME, ASTM, ASSE, CSA, NSF,
UL, and others.
The
CE Mark indicates compliance to the
applicable requirements of a particular
product as outlined by the International
Electrotechnical Commission (IEC) and by
mutual agreement is recognized throughout
the European Union. Micron has utilized
the Canadian Standards Association (CSA)
as a competent body in reviewing, interpreting
and properly complying with the requirements
to place a CE mark on its GlobalTRAN product.
As a national certification body, CSA also
has the proper documentation and reports
on file for GlobalTRAN to utilize the CB
Scheme, ensuring acceptance throughout the
world.
In
addition to the CE mark, a Declaration of
Conformity may be required by some customs
agencies. Micron will furnish copies of
this Declaration upon request. Copies of
the related CB Test Certificate and CSA
Letter of Attestation are also available.
The standard GlobalTRAN product is supplied
with terminal covers which meets the requirements
of IEC-529 IP20 degree of protection.
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Transformer
Classifications |
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Transformers
are adapted to numerous engineering applications
and may be classified in many ways:
*
By power level (from fraction of a volt-ampere(VA)
to over a thousand MVA),
* By application (power supply, impedance
matching, circuit isolation),
* By frequency range (power, audio, radio
frequency(RF))
* By voltage class (a few volts to about
750 kilovolts)
* By cooling type (air cooled, oil filled,
fan cooled, water cooled, etc.)
* By purpose (distribution, rectifier, arc
furnace, amplifier output, etc.).
* By ratio of the number of turns in the
coils
Step-up
The
secondary has more turns than the primary.
Step-down
The secondary has fewer turns than the primary.
Isolating
Intended to transform from one voltage to
the same voltage. The two coils have approximately
equal numbers of turns, although often there
is a slight difference in the number of
turns, in order to compensate for losses
(otherwise the output voltage would be a
little less than, rather than the same as,
the input voltage).
Variable
The primary and secondary have an adjustable
number of turns which can be selected without
reconnecting the transformer.
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Transformer
Limitations and Energy Losses |
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Limitations
Transformers
alone cannot do the following:
* Convert DC to AC or vice versa
* Change the voltage or current of DC
* Change the AC supply frequency.
However,
transformers are components of the systems
that perform all these functions.
Energy
Losses
An
ideal transformer would have no losses,
and would therefore be 100% efficient. In
practice, energy is dissipated due both
to the resistance of the windings known
as copper loss or I2 R loss, and to magnetic
effects primarily attributable to the core
(known as iron loss measured in watts per
pound). Transformers are, in general, highly
efficient. Large power transformers (over
50 MVA) may attain an efficiency as high
as 99.75%. Small transformers, such as a
plug-in "power brick" used to
power small consumer electronics, may be
less than 85% efficient.
Transformer
losses arise from:
* Winding resistance
Current
flowing through the windings causes resistive
heating of the conductors (I2 R loss). At
higher frequencies, skin effect and proximity
effect create additional winding resistance
and losses.
* Eddy currents
Induced
eddy currents circulate within the core,
causing resistive heating. Silicon is added
to the steel to help in controlling eddy
currents. Adding silicon also has the advantage
of stopping aging of the electrical steel
that was a problem years ago.
* Hysteresis losses
Each
time the magnetic field is reversed, a small
amount of energy is lost to hysteresis within
the magnetic core. The amount of hysteresis
is a function of the particular core material.
* Magnetostriction
Magnetic
flux in the core causes it to physically
expand and contract slightly with the alternating
magnetic field, an effect known as magnetostriction.
This in turn causes losses due to frictional
heating in susceptible ferromagnetic cores.
* Mechanical losses
In
addition to magnetostriction, the alternating
magnetic field causes fluctuating electromagnetic
forces between the primary and secondary
windings. These incite vibrations within
nearby metalwork, creating a familiar humming
or buzzing noise, and consuming a small
amount of power.
* Stray losses
Not
all the magnetic field produced by the primary
is intercepted by the secondary. A portion
of the leakage flux may induce eddy currents
within nearby conductive objects, such as
the transformer's support structure, and
be converted to heat.
* Cooling system
Large
power transformers may be equipped with
cooling fans, oil pumps or water-cooled
heat exchangers designed to remove the heat
caused by copper and iron losses. The power
used to operate the cooling system is typically
considered part of the losses of the transformer.
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Cores
Laminate Steel cores
Transformers
for use at power or audio frequencies have
cores made of many thin laminations of silicon
steel. By concentrating the magnetic flux,
more of it is usefully linked by both primary
and secondary windings. Since the steel
core is conductive, it, too, has currents
induced in it by the changing magnetic flux.
Each layer is insulated from the adjacent
layer to reduce the energy lost to eddy
current heating of the core. The thin laminations
are used to reduce the eddy currents, and
the insulation is used to keep the laminations
from acting as a solid piece of steel. The
thinner the laminations, the lower the eddy
currents, and the lower the losses. Very
thin laminations are generally used on high
frequency transformers. The cost goes up
when using thinner laminations mainly over
the labor in stacking them. A typical laminated
core is made from E-shaped and I-shaped
pieces, leading to the name "EI transformer".
In the EI transformer, the laminations are
stacked in what is known as an interleaved
fashion. Due to this interleaving a second
gap in parallel (in an analogy to electronic
circuits) to the gap between E and I is
formed between the E-pieces. The E-pieces
are pressed together to reduce the gap width
to that of the insulation. The gap area
is very large, so that the effective gap
width is very small (in analogy to a capacitor).
For this to work the flux has to gradually
flow from one E to the other. That means
that on one end all flux is only on every
second E. That means saturation occurs at
half the flux density. Using a longer E
and wedging it with two small Is will increase
the overlap and additionally make the grains
more parallel to the flux (think of a wooden
frame for a window). If an air gap is needed
(which is unlikely considering the low remanence
available for steel), all the E's are stacked
on one side, and all the I's on the other
creating a gap.
The
cut core or C-core is made by winding a
silicon steel strip around a rectangular
form. After the required thickness is achieved,
it is removed from the form and the laminations
are bonded together. It is then cut in two
forming two C shapes. The faces of the cuts
are then ground smooth so they fit very
tight with a very small gap to reduce losses.
The core is then assembled by placing the
two C halves together, and holding them
closed by a steel strap. Usually two C-cores
are used to shorten the return path for
the magnetic flux resulting in a form similar
to the EI. More cores would necessitate
a triangular cross-section. Like toroidal
cores they have the advantage, that the
flux is always in the oriented parallel
the grains. Due to the bending of the core
some area is lost for a rectangular winging.
A steel core's remanence means that it retains
a static magnetic field when power is removed.
When power is then reapplied, the residual
field will cause a high inrush current until
the effect of the remanent magnetism is
reduced, usually after a few cycles of the
applied alternating current. Overcurrent
protection devices such as fuses must be
selected to allow this harmless inrush to
pass. On transformers connected to long
overhead power transmission lines, induced
currents due to geomagnetic disturbances
during solar storms can cause saturation
of the core, and false operation of transformer
protection devices. Steel cores develop
a larger hysteresis loss due to eddy currents
as the operating frequency is increased.
Ferrite, or thinner steel laminations for
the core are typically used for frequencies
above 1kHz. The thinner steel laminations
serve to reduce the eddy currents. Some
types of very thin steel laminations can
operate at up to 10 kHz or higher. Ferrite
is used in higher frequency applications,
extending to the VHF band and beyond. Aircraft
traditionally use 400 Hz power systems since
the slight increase in thermal losses is
more than offset by the reduction in core
and winding weight. Military gear includes
400 Hz (and other frequencies) to supply
power for radar or servomechanisms.
Distribution
transformers can achieve low off-load losses
by using cores made with low loss high permeability
silicon steel and amorphous (non-crystalline)
steel, so-called "metal glasses"
the high cost of the core material
is offset by the lower losses incurred at
light load, over the life of the transformer.
In order to maintain good voltage regulation,
distribution transformers are designed to
have very low leakage inductance.
Certain
special purpose transformers use long magnetic
paths, insert air gaps, or add magnetic
shunts (which bypass a portion of magnetic
flux that would otherwise link the primary
and secondary windings) in order to intentionally
add leakage inductance. The additional leakage
inductance limits the secondary winding's
short circuit current to a safe, or a controlled,
level. This technique is used to stabilize
the output current for loads that exhibit
negative resistance such as electric arcs,
mercury vapor lamps, and neon signs, or
safely handle loads that may become periodically
short-circuited such as electric arc welders.
Gaps are also used to keep a transformer
from saturating, especially audio transformers
which have a DC component added.
Solid
cores
Powdered
iron cores are used in circuits (such as
switch-mode power supplies) that operate
above mains frequencies and up to a few
tens of kilohertz. These materials combine
high magnetic permeability with high bulk
electrical resistivity. At even higher,
radio-frequencies (RF), other types of cores
made from non-conductive magnetic ceramic
materials, called ferrites, are common.
Some RF transformers also have moveable
cores (sometimes called slugs) which allow
adjustment of the coupling coefficient (and
bandwidth) of tuned radio-frequency circuits.
Cores are available in a wide variety of
shapes, including toroids. Other shapes
include so-called E-cores and C-cores.
Air cores
High-frequency
transformers may also use air cores. These
eliminate the loss due to hysteresis in
the core material. Such transformers maintain
high coupling efficiency (low stray field
loss) by overlapping the primary and secondary
windings.
Toroidal
cores
Toroidal
transformers are built around a ring-shaped
core, which is made from a long strip of
silicon steel or permalloy wound into a
coil, from powdered iron, or ferrite, depending
on operating frequency. The strip construction
ensures that the grain boundaries are optimally
aligned, improving the transformer's efficiency
by reducing the core's reluctance. The closed
ring shape eliminates air gaps inherent
in the construction of an EI core. The cross-section
of the ring is usually square or rectangular,
but more expensive cores with circular cross-sections
are also available. The primary and secondary
coils are often wound concentrically to
cover the entire surface of the core. This
minimises the length of wire needed, and
also provides screening to minimize the
core's magnetic field from generating electromagnetic
interference. Ferrite toroid cores are used
at higher frequencies, typically between
a few tens of kilohertz to a megahertz,
to reduce losses, physical size, and weight
of switch-mode power supplies. Toroidal
transformers are more efficient than the
cheaper laminated EI types of similar power
level. Other advantages, compared to EI
types, include smaller size (about half),
lower weight (about half), less mechanical
hum (making them superior in audio amplifiers),
lower exterior magnetic field (about one
tenth), low off-load losses (making them
more efficient in standby circuits), single-bolt
mounting, and more choice of shapes. This
last point means that, for a given power
output, either a wide, flat toroid or a
tall, narrow one with the same electrical
properties can be chosen, depending on the
space available. The main disadvantages
are higher cost and limited size. A drawback
of toroidal transformer construction is
the higher cost of windings. As a consequence,
toroidal transformers are uncommon above
ratings of a few kVA. Small distribution
transformers may achieve some of the benefits
of a toroidal core by splitting it and forcing
it open, then inserting a bobbin containing
primary and secondary windings. When fitting
a toroidal transformer, it is important
to avoid making an unintentional short-circuit
through the core. This can happen if the
steel mounting bolt in the middle of the
core is allowed to touch metalwork at both
ends, making a loop of conductive material
which passes through the hole in the toroid.
Such a loop could result in a dangerously
large current flowing in the bolt.
Windings
The
wire of the adjacent turns in a coil, and
in the different windings, must be electrically
insulated from each other. The wire used
is generally magnet wire. Magnet wire is
a copper wire with a coating of varnish
or some other synthetic coating. Transformers
for years have used Formvar wire which is
a varnished type of magnet wire. The conducting
material used for the winding depends upon
the application. Small power and signal
transformers are wound with solid copper
wire, insulated usually with enamel, and
sometimes additional insulation. Larger
power transformers may be wound with wire,
copper, or aluminum rectangular conductors.
Strip conductors are used for very heavy
currents. High frequency transformers operating
in the tens to hundreds of kilohertz will
have windings made of Litz wire to minimize
the skin effect losses in the conductors.
Large power transformers use multiple-stranded
conductors as well, since even at low power
frequencies non-uniform distribution of
current would otherwise exist in high-current
windings. Each strand is insulated from
the other, and the strands are arranged
so that at certain points in the winding,
or throughout the whole winding, each portion
occupies different relative positions in
the complete conductor. This "transposition"
equalizes the current flowing in each strand
of the conductor, and reduces eddy current
losses in the winding itself. The stranded
conductor is also more flexible than a solid
conductor of similar size. For signal transformers,
the windings may be arranged in a way to
minimise leakage inductance and stray capacitance
to improve high-frequency response. This
can be done by splitting up each coil into
sections, and those sections placed in layers
between the sections of the other winding.
This is known as a stacked type or interleaved
winding. Windings on both the primary and
secondary of power transformers may have
external connections (called taps) to intermediate
points on the winding to allow adjustment
of the voltage ratio. Taps may be connected
to an automatic, on-load tap changer type
of switchgear for voltage regulation of
distribution circuits. Audio-frequency transformers,
used for the distribution of audio to public
address loudspeakers, have taps to allow
adjustment of impedance to each speaker.
A center-tapped transformer is often used
in the output stage of an audio power amplifier
in a push-pull type circuit. Modulation
transformers in AM transmitters are very
similar. Tapped transformers are also used
as components of amplifiers, oscillators,
and for feedback linearization of amplifier
circuits.
Insulation
The
turns of the windings must be insulated
from each other to ensure that the current
travels through the entire winding. The
potential difference between adjacent turns
is usually small, so that enamel insulation
is usually sufficient for small power transformers.
Supplemental sheet or tape insulation is
usually employed between winding layers
in larger transformers. The transformer
may also be immersed in transformer oil
that provides further insulation. Although
the oil is primarily used to cool the transformer,
it also helps to reduce the formation of
corona discharge within high voltage transformers.
By cooling the windings, the insulation
will not break down as easily due to heat.
To ensure that the insulating capability
of the transformer oil does not deteriorate,
the transformer casing is completely sealed
against moisture ingress. Thus the oil serves
as both a cooling medium to remove heat
from the core and coil, and as part of the
insulation system. Certain power transformers
have the windings protected by epoxy resin.
By impregnating the transformer with epoxy
under a vacuum, air spaces within the windings
are replaced with epoxy, thereby sealing
the windings and helping to prevent the
possible formation of corona and absorption
of dirt or water. This produces transformers
suitable for damp or dirty environments,
but at increased manufacturing cost.
Shielding
Where
transformers are intended for minimum electrostatic
coupling between primary and secondary circuits,
an electrostatic shield can be placed between
windings to reduce the capacitance between
primary and secondary windings. The shield
may be a single layer of metal foil, insulated
where it overlaps to prevent it acting as
a shorted turn, or a single layer winding
between primary and secondary. The shield
is connected to earth ground. Transformers
may also be enclosed by magnetic shields,
electrostatic shields, or both to prevent
outside interference from affecting the
operation of the transformer, or to prevent
the transformer from affecting the operation
of nearby devices that may be sensitive
to stray fields such as CRTs.
Coolant
Small
signal transformers do not generate significant
amounts of heat. Power transformers rated
up to a few kilowatts rely on natural convective
air cooling. Specific provision must be
made for cooling of high-power transformers.
Transformers handling higher power, or having
a high duty cycle can be fan-cooled.
The
windings of high-power or high-voltage transformers
are immersed in transformer oil a
highly-refined mineral oil, that is stable
at high temperatures. Large transformers
to be used indoors must use a non-flammable
liquid. Formerly, polychlorinated biphenyl
(PCB) was used as it was not a fire hazard
in indoor power transformers and it is highly
stable. Due to the stability and toxic effects
of PCB byproducts, and its accumulation
in the environment, it is no longer permitted
in new equipment. Old transformers which
still contain PCB should be examined on
a weekly basis for leakage. If found to
be leaking, it should be changed out, and
professionally decontaminated or scrapped
in an environmentally safe manner. Today,
nontoxic, stable silicone-based oils, or
fluorinated hydrocarbons may be used where
the expense of a fire-resistant liquid offsets
additional building cost for a transformer
vault. Other less-flammable fluids such
as canola oil may be used but all fire resistant
fluids have some drawbacks in performance,
cost, or toxicity compared with mineral
oil. The oil cools the transformer, and
provides part of the electrical insulation
between internal live parts. It has to be
stable at high temperatures so that a small
short or arc will not cause a breakdown
or fire. The oil-filled tank may have radiators
through which the oil circulates by natural
convection. Very large or high-power transformers
(with capacities of millions of watts) may
have cooling fans, oil pumps and even oil
to water heat exchangers. Oil-filled transformers
undergo prolonged drying processes, using
vapor-phase heat transfer, electrical self-heating,
the application of a vacuum, or combinations
of these, to ensure that the transformer
is completely free of water vapor before
the cooling oil is introduced. This helps
prevent electrical breakdown under load.
Oil-filled power transformers may be equipped
with Buchholz relays which are safety devices
that sense gas build-up inside the transformer
(a side effect of an electric arc inside
the windings), and thus switches off the
transformer.
Terminals
Very
small transformers will have wire leads
connected directly to the ends of the coils,
and brought out to the base of the unit
for circuit connections. Larger transformers
may have heavy bolted terminals, bus bars
or high-voltage insulated bushings made
of polymers or porcelain. A large bushing
can be a complex structure since it must
provide electrical insulation without letting
the transformer leak oil.
Enclosure
Small
transformers often have no enclosure. Transformers
may have a shield enclosure, as described
above. Larger units may be enclosed to prevent
contact with live parts, and to contain
the cooling medium (oil or pressurized gas).
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Transformer
Types and Uses |
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Autotransformers
An autotransformer has only a single winding,
which is tapped at some point along the
winding. AC or pulsed voltage is applied
across a portion of the winding, and a
higher (or lower) voltage is produced
across another portion of the same winding.
While theoretically separate parts of
the winding can be used for input and
output, in practice the higher voltage
will be connected to the ends of the winding,
and the lower voltage from one end to
a tap. For example, a transformer with
a tap at the center of the winding can
be used with 230 volts across the entire
winding, and 115 volts between one end
and the tap. It can be connected to a
230 volt supply to drive 115 volt equipment,
or reversed to drive 230 volt equipment
from 115 volts. As the same winding is
used for input and output, the flux in
the core is partially cancelled, and a
smaller core can be used. For voltage
ratios not exceeding about 3:1, an autotransformer
is cheaper, lighter, smaller and more
efficient than a true (two-winding) transformer
of the same rating. In practice, transformer
losses mean that autotransformers are
not perfectly reversible; one designed
for stepping down a voltage will deliver
slightly less voltage than required if
used to step up. The difference is usually
slight enough to allow reversal where
the actual voltage level is not critical.
By exposing part of the winding coils
and making the secondary connection through
a sliding brush, an autotransformer with
a near-continuously variable turns ratio
can be obtained, allowing for very small
increments of voltage.
Polyphase
transformers
For
three-phase power, three separate single-phase
transformers can be used, or all three
phases can be connected to a single polyphase
transformer. The three primary windings
are connected together and the three secondary
windings are connected together. The most
common connections are Y-?, ?-Y, ?-? and
Y-Y. A vector group indicates the configuration
of the windings and the phase angle difference
between them. If a winding is connected
to earth (grounded), the earth connection
point is usually the center point of a
Y winding. If the secondary is a ? winding,
the ground may be connected to a center
tap on one winding (high leg delta) or
one phase may be grounded (corner grounded
delta). A special purpose polyphase transformer
is the zigzag transformer. There are many
possible configurations that may involve
more or fewer than six windings and various
tap connections.
Variable Frequency Transformer
The
variable frequency transformer (VFT) is
a continuously variable phase-shifting
transformer that can operate at an adjustable
phase angle. The core technology of the
VFT is a rotary transformer with three-phase
windings on both rotor and stator.
The
collector system conducts current between
the three-phase rotor winding and its
stationary buswork. One power grid is
connected to the rotor side of the VFT
and the other to the stator side. Power
flow is proportional to the angle of the
rotary transformer, as with any other
ac power circuit. The impedance of the
rotary transformer and ac grid determine
the magnitude of phase shift required
for a given power transfer. Power transfer
through the rotary transformer is a function
of the torque applied to the rotor. If
torque is applied in one direction, then
power flows from the stator winding to
the rotor winding. If torque is applied
in the opposite direction, then power
flows from the rotor winding to the stator
winding. Power flow is proportional to
the magnitude and direction of the torque
applied. If no torque is applied, then
no power flows through the rotary transformer.
Regardless of power flow, the rotor inherently
orients itself to follow the phase angle
difference imposed by the two asynchronous
systems and will rotate continuously if
the grids are at different frequencies.
Torque
is applied to the rotor by a drive motor,
which is controlled by the variable-speed
drive system. When a VFT is used to interconnect
two power grids of the same frequency,
its normal operating speed is zero. Therefore,
the motor/drive system is designed to
continuously produce torque while at zero
speed (standstill). However, if the power
grid on one side experiences a disturbance
that causes a frequency excursion, the
VFT will rotate at a speed proportional
to the difference in frequency between
the two power grids. During this operation,
the load flow is maintained. The VFT is
designed to continuously regulate power
flow with drifting frequencies on both
grids. A closed-loop power regulator maintains
power transfer equal to an operator setpoint.
The regulator compares measured power
with the setpoint and adjusts motor torque
as a function of power error. The power
regulator is fast enough to respond to
network disturbances and to maintain stable
power transfer.
Resonant
transformers
A
resonant transformer operates at the resonant
frequency of one or more of its coils
and (usually) an external capacitor. The
resonant coil, usually the secondary,
acts as an inductor, and is connected
in series with a capacitor. When the primary
coil is driven by a periodic source of
alternating current, such as a square
or Sawtooth wave at the resonant frequency,
each pulse of current helps to build up
an oscillation in the secondary coil.
Due to resonance, a very high voltage
can develop across the secondary, until
it is limited by some process such as
electrical breakdown. These devices are
used to generate high alternating voltages,
and the current available can be much
larger than that from electrostatic machines.
Examples:
* Tesla coil
* Oudin coil (or Oudin resonator; named
after its inventor Paul Oudin)
* D'Arsonval apparatus
* Ignition coil or induction coil used
in the ignition system of a petrol engine
* Flyback transformer of a CRT television
set or video monitor.
* Electrical breakdown and insulation
testing of high voltage equipment and
cables. In the latter case, the transformer's
secondary is resonated with the cable's
capacitance.
Other
applications of resonant transformers
are as coupling between stages of a superheterodyne
receiver, where the selectivity of the
receiver is provided by the tuned transformers
of the intermediate-frequency amplifiers.
A
voltage regulating transformer uses a
resonant winding and allows part of the
core to go into saturation on each half-cycle
of the alternating current. This effect
stabilizes the output of the regulating
transformer, which can be used for equipment
that is sensitive to variations of the
supply voltage. Saturating transformers
provide a simple rugged method to stabilize
an AC power supply. However, due to the
hysteresis losses accompanying this type
of operation, efficiency is low.
Current transformers
A
current transformer is a type of "instrument
transformer" that is designed to
provide a current in its secondary which
is accurately proportional to the current
flowing in its primary. This accuracy
is directly related to a number of factors
including the following:
* burden,
* rating factor,
* load,
* external electromagnetic fields,
* temperature and
* physical CT configuration.
The
burden in a CT metering circuit is essentially
the amount of impedance (largely resistive)
present. Typical burden ratings for CTs
are B-0.1, B-0.2, B-0.5, B-1.0, B-2.0
and B-4.0. This means a CT with a burden
rating of B-0.2 can tolerate up to 0.2?
of impedance in the metering circuit before
its output current is no longer a fixed
ratio to the primary current. Items that
contribute to the burden of a current
measurement circuit are switch blocks
meters and intermediate conductors. The
most common source of excess burden in
a current measurement circuit is the conductor
between the meter and the CT. Often times,
substation meters are located significant
distances from the meter cabinets and
the excessive length of small gauge conductor
creates a large resistance.
Rating
factor is a factor by which the nominal
full load current of a CT can be multiplied
to determine its absolute maximum measurable
primary current. Conversely, the minimum
primary current a CT can accurately measure
is "light load," or 10% of the
nominal current. The rating factor of
a CT is largely dependent upon ambient
temperature. Most CTs have rating factors
for 35 degrees Celsius and 55 degrees
Celsius. A CT usually demonstrates reduced
capacity to maintain accuracy with rising
ambient temperature. It is important to
be mindful of ambient temperatures and
resultant rating factors when CTs are
installed inside pad-mounted transformers
or poorly ventilated mechanical rooms.
Recently, manufacturers have been moving
towards lower nominal primary currents
with greater rating factors. This is made
possible by the development of more efficient
ferrites and their corresponding hysteresis
curves. This is a distinct advantage over
previous CTs because it increases their
range of accuracy. For example, a 200:5
CT with a rating factor of 4.0 is most
accurate between 20A (light load)and 800A
(4.0 times the nominal rating, or "full
load," of the CT) of primary current.
While previous revisions of CTs were on
the order of 500:5 with a rating factor
of 1.5 yielding an effective range of
50A to 750A. This is an 11% increase in
effective range for two CTs that would
be used at similar services. Not to mention,
the relative cost of a 500:5 CT is significantly
greater than that of a 200:5.
Physical
CT configuration is another important
factor in reliable CT accuracy. While
all electrical engineers are quite comfortable
with Gauss' Law, there are some issues
when attempting to apply theory to the
real world. When conductors passing through
a CT are not centered in the circular
(or oval) void, slight inaccuracies may
occur. It is important to center primary
conductors as they pass through CTs to
promote the greatest level of CT accuracy.
Afterall, in an electric metering circuit,
the most inaccurate component is the CT.
Current transformers (CTs) are commonly
used in metering and protective relaying
in the electrical power industry where
they facilitate the safe measurement of
large currents, often in the presence
of high voltages. The current transformer
safely isolates measurement and control
circuitry from the high voltages typically
present on the circuit being measured.
Current
transformers are often constructed by
passing a single primary turn (either
an insulated cable or an uninsulated bus
bar) through a well-insulated toroidal
core wrapped with many turns of wire.
Current transformers are used extensively
for measuring current and monitoring the
operation of the power grid. The CT is
typically described by its current ratio
from primary to secondary. Common secondaries
are 1 or 5 amperes. For example, a 4000:5
CT would provide an output current of
5 amperes when the primary was passing
4000 amperes. The secondary winding can
be single ratio or multi ratio, with five
taps being common for multi ratio CTs.
Typically, the secondary connection points
are labeled as 1s1, 1s2, 2s1, 2s2 and
so on. The multi ratio CTs are typically
used for current matching in current differential
protective relaying applications. Often,
multiple CTs will be installed as a "stack"
for various uses (for example, protection
devices and revenue metering may use separate
CTs). For a three-stacked CT application,
the secondary winding connection points
are typically labeled Xn, Yn, Zn. Care
must be taken that the secondary of a
current transformer is not disconnected
from its load while current is flowing
in the primary, as this will produce a
dangerously high voltage across the open
secondary. Specially constructed wideband
current transformers are also used (usually
with an oscilloscope) to measure waveforms
of high frequency or pulsed currents within
pulsed power systems. One type of specially
constructed wideband transformer provides
a voltage output that is proportional
to the measured current. Another type
(called a Rogowski coil) requires an external
integrator in order to provide a voltage
output that is proportional to the measured
current. Unlike CTs used for power circuitry,
wideband CT's are rated in output volts
per ampere of primary current.
Voltage
transformers
Voltage
transformers (VTs) or potential transformers
(PTs) are another type of instrument transformer,
used for metering and protection in high-voltage
circuits. They are designed to present
negligible load to the supply being measured
and to have a precise voltage ratio to
accurately step down high voltages so
that metering and protective relay equipment
can be operated at a lower potential.
Typically the secondary of a voltage transformer
is rated for 69 or 120 Volts at rated
primary voltage, to match the input ratings
of protection relays. The transformer
winding high-voltage connection points
are typically labelled as H1, H2 (sometimes
H0 if it is internally grounded) and X1,
X2, and sometimes an X3 tap may be present.
Sometimes a second isolated winding (Y1,
Y2, Y3) may also be available on the same
voltage transformer. The high side (primary)
may be connected phase to ground or phase
to phase. The low side (secondary) is
usually phase to ground. The terminal
identifications (H1, X1, Y1, etc.) are
often referred to as polarity. This applies
to current transformers as well. At any
instant terminals with the same suffix
numeral have the same polarity and phase.
Correct identification of terminals and
wiring is essential for proper operation
of metering and protection relays. While
VTs were formerly used for all voltages
greater than 240V primary, modern meters
eliminate the need VTs for most secondary
service voltages. For new, or rework,
meter packages, VTs are typically only
installed in primary voltage (typically
12.5kV) or generation voltage (13.2kV)
meter packages.
Pulse transformers
A
pulse transformer is a transformer that
is optimised for transmitting rectangular
electrical pulses (that is, pulses with
fast rise and fall times and a constant
amplitude). Small versions called signal
types are used in digital logic and telecommunications
circuits, often for matching logic drivers
to transmission lines. Medium-sized power
versions are used in power-control circuits
such as camera flash controllers. Larger
power versions are used in the electrical
power distribution industry to interface
low-voltage control circuitry to the high-voltage
gates of power semiconductors. Special
high voltage pulse transformers are also
used to generate high power pulses for
radar, particle accelerators, or other
high energy pulsed power applications.
To minimize distortion of the pulse shape,
a pulse transformer needs to have low
values of leakage inductance and distributed
capacitance, and a high open-circuit inductance.
In power-type pulse transformers, a low
coupling capacitance (between the primary
and secondary) is important to protect
the circuitry on the primary side from
high-powered transients created by the
load. For the same reason, high insulation
resistance and high breakdown voltage
are required. A good transient response
is necessary to maintain the rectangular
pulse shape at the secondary, because
a pulse with slow edges would create switching
losses in the power semiconductors. The
product of the peak pulse voltage and
the duration of the pulse (or more accurately,
the voltage-time integral) is often used
to characterise pulse transformers. Generally
speaking, the larger this product, the
larger and more expensive the transformer.
RF
transformers (transmission line
transformers)
For
radio frequency use, transformers are
sometimes made from configurations of
transmission line, sometimes bifilar or
coaxial cable, wound around ferrite or
other types of core. This style of transformer
gives an extremely wide bandwidth but
only a limited number of ratios (such
as 1:9, 1:4 or 1:2) can be achieved with
this technique. The core material increases
the inductance dramatically, thereby raising
its Q factor. The cores of such transformers
help improve performance at the lower
frequency end of the band. RF transformers
sometimes used a third coil (called a
tickler winding) to inject feedback into
an earlier (detector) stage in antique
regenerative radio receivers.
Baluns
Baluns
are transformers designed specifially
to connect between balanced and unbalanced
circuits. These are sometimes made from
configurations of transmission line and
sometimes bifilar or coaxial cable and
are similar to transmission line transformers
in construction and operation.
Audio
transformers
Transformers in a tube amplifier. Output
transformers are on the left. The power
supply toroidal transformer is on right.
Audio transformers are usually the factor
which limit sound quality; electronic
circuits with wide frequency response
and low distortion are relatively simple
to design. Transformers are also used
in DI boxes to convert impedance from
high-impedance instruments (for example,
bass guitars) to enable them to be connected
to a microphone input on the mixing console.
A particularly critical component is the
output transformer of an audio power amplifier.
Valve circuits for quality reproduction
have long been produced with no other
(inter-stage) audio transformers, but
an output transformer is needed to couple
the relatively high impedance (up to a
few hundred ohms depending upon configuration)
of the output valve(s) to the low impedance
of a loudspeaker. (The valves can deliver
a low current at a high voltage; the speakers
require high current at low voltage.)
Solid-state power amplifiers may need
no output transformer at all. For good
low-frequency response a relatively large
iron core is required; high power handling
increases the required core size. Good
high-frequency response requires carefully
designed and implemented windings without
excessive leakage inductance or stray
capacitance. All this makes for an expensive
component.
Speaker transformers
In
the same way that transformers are used
to create high voltage power transmission
circuits that minimize transmission losses,
speaker transformers allow many individual
loudspeakers to be powered from a single
audio circuit operated at higher-than
normal speaker voltages. This application
is common in public address (e.g., Tannoy)
applications. Such circuits are commonly
referred to as constant voltage or 70
volt speaker circuits although the audio
waveform is obviously a constantly changing
voltage. At the audio amplifier, a large
audio transformer may be used to step-up
the low impedance, low-voltage output
of the amplifier to the designed line
voltage of the speaker circuit. Then,
a smaller transformer at each speaker
returns the voltage and impedance to ordinary
speaker levels. The speaker transformers
commonly have multiple primary taps, allowing
the volume at each speaker to be adjusted
in a number of discrete steps. Use of
a constant-voltage speaker circuit means
that there is no need to worry about the
impedance presented to the amplifier output
(which would clearly be too low if all
of the speakers were arranged in parallel
and would be too complex a design problem
if the speakers were arranged in series-parallel).
The use of higher transmission voltage
and impedance means that power lost in
the connecting wire is minimized, even
with the use of small-gauge conductors
(and leads to the term constant voltage
as the line voltage doesn't change much
as additional speakers are added to the
system). Also, the ability to adjust,
locally, the volume of each speaker (without
the complexity and power loss of an L
pad) is a useful feature.
Additional
Information:
General
Transfomer FAQ - http://www.microntransformers.com/support/faq_control.php
Basic
Transformer Wiring - http://www.hammondmfg.com/5CHook.htm
Transformer
Sizing Guide
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