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Dielectric
In reality
the dielectric is not an ideal insulator, i.e. a certain
number of electrons penetrate it.
Due to these processes and also to changing polarization
in the material, part of the electric energy is lost as
dissipated heat: |
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a)
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Ohmic
losses: there is a difference between insulation
resistance = volume resistance Rv
(current flow through the interior of the
insulator) and surface resistance = the external
resistance Rs (current flow over the surface of
the insulator due to humidity or dirt). Together
they make up the complete resistance |
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| The ohmic
losses are to be seen in the rise of the temperature of
the insulator which is often quite considerable. |
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| b) |
Dielectric
losses (dissipation) are the result of
the changing polarization of the elementary
particles of the dielectric caused by alternating
fields.
They are transformed into oscillations (like
little compass needles) and thus produce
frictional heat. So, here too, part of the
electric energy is lost in heat. |
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| The losses amount to: |
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tan is the dissipation factor,
it is the measurement of dielectric losses and is
dependent on frequency.
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