Transformer Losses-all types
An
Ideal transformer have no energy losses i.e zero losses, and 100% efficient. but in real (In practical) transformers, energy is dissipated in the windings, core, and surrounding structures. Larger transformers are generally more efficient, and those of distribution transformer usually perform better than 98%.
Experimental transformers using superconducting ( Super conductor is one that in which zero losses occur) windings achieve efficiencies of 99.85% but it will be available in coming years.
Ideal transformer have no energy losses i.e zero losses, and 100% efficient. but in real (In practical) transformers, energy is dissipated in the windings, core, and surrounding structures. Larger transformers are generally more efficient, and those of distribution transformer usually perform better than 98%.
The different losses in the transformer
1.copper losses (Winding resistance)
Current
flowing through the windings causes resistive heating of the
conductors. At higher frequencies, skin effect and proximity effect
create additional winding resistance and losses.
Total cupper losses = I12. R1+ I22R2 = I12. R 01+ I22R 02
2.Core or Iron Losses
There are two types of core or iron losses as follows:
2.1) Hysteresis losses
Each time the magnetic field is reversed, a small amount of energy is lost due to hysteresis within the
core. For a given core material, the loss is proportional to the
frequency, and is a function of the peak flux density to which it is
subjected.
We can find Hysteresis losses by this formula.
Wh = ηB1.6maxf.v watt
2.2) Eddy currents
Ferromagnetic
materials are also good conductors, and a core made from such a
material also constitutes a single short-circuited turn throughout its
entire length.Eddy currents therefore,
circulates
within the core in a plane normal to the flux, and are responsible for
resistive heating of the core material.The eddy current loss is a
complex function of the square of supply frequency and inverse square of
the material thickness. Eddy current losses can be reduced by making
the core of a stack of plates electrically insulated from each other,
rather than a solid block; all transformers operating at low frequencies
use laminated or similar cores.
We can find Eddy currents losses by this formula.
We = PB2max.f2t2 Watt
3.Magnetostriction
Magnetic
flux in a ferromagnetic material, such as the core, causes it to
physically expand and contract slightly with each cycle of the magnetic
field, an effect known as magnetostriction. This produces the buzzing
sound commonly associated with transformers, and can cause losses due to
frictional heating.
Mechanical losses
In addition to magnetostriction, the alternating magnetic field causes fluctuating forces between the primary and secondary windings. These incite vibrations within nearby metalwork, adding to the buzzing noise, and consuming a small amount of power.
Stray losses (leakage Flux)
Leakage
inductance is by itself largely lossless, since energy supplied to its
magnetic fields is returned to the supply with the next half-cycle.
However, any leakage flux that intercepts nearby conductive materials
such as the transformer’s support structure will give rise to eddy
currents and be converted to heat. There are also radiative losses due
to the oscillating magnetic field, but these are usually small.
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