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Electromagnetic energy is converted to thermal energy, causing
wave attenuation and material heating.
The affect of losses on the propagating wave is due to the materials
response to either the electric or magnetic field. In most cases it is
usually the electric field that produces a response. This response can
be attributed to two main dielectric mechanisms: ionic polarisation and
dipole rotation. There are other mechanisms which can dominate in certain
situations, however we are mainly concerned with ionic polarisation and
dipole rotation since industrial microwave systems usually involves heating
of liquids and non magnetic solids.
As the wave progresses into a lossy material, its amplitude decreases
due to the transfer of energy as heat into the material. The field and
power flux density falls exponentially with distance from the surface.
The rate of decay is proportional to the materials dielectric properties
and the wave frequency. The depth of penetration is defined as the distance
into the material at which the power flux has fallen to 1/e(=0.368) of
its surface value. The wave still penetrates beyond this point however
the power flux density is a value less than 0.368 of that on the surface.
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Skin Depth
Skin depth is not the same as penetration
depth. It refers to the surface skin of a conducting wall in
which the majority of current flows. As microwave energy encounters
a conductor, nearly all the energy is reflected from the wall
and only a very small proportion is absorbed.
Frequency Dependance
It should be noted that frequency is an
important factor in determining whether a medium acts like a
lossy dielectric or a conductor.
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