The radiation abundant in nature and man-made is classified into many types. The
types of man-made radiation are listed in Tables 1a and
1b, along with their respective domain frequencies and wavelengths. Of these, the frequency domain from 1 Hz to 300 GHz
is of great interest to us as the entire gamut of the telecommunication
range, starting from the AM radio and extending up to the telemetry waves,
X band and W band microwaves, falls within this range. Because of their
widespread use in telecommunications, their widespread
interaction with the human body assumes significance.
The Radio-Frequency (RF) waves, microwaves and the millimeter waves used
for telemetry and cooking are categorized as non-ionizing as they do not have
sufficient quantum energy to ionize an atom, meaning they cannot eject electrons from an atom
or molecule to produce a positively charged core or ion. The threshold for ionization
occurs somewhere in the ultraviolet range. However, in the RF and microwaves
range, the radiation just contributes to the random molecular
motion, which can be described as thermal energy. As an indirect effect of the heating phenomenon, chemical changes
are likely to occur in the human body (Nave and Nave, 1985). To have a physiological
effect, the energy of the radiation must be
absorbed. To be absorbed, there must be quantum energy level pairs which match the
photon energy of the radiation. Further, the
dielectric constant of the material must also be high
in order to absorb the radiation to which it is
exposed. A low dielectric constant for the material means good transmission, low
loss, low capacitance and low absorption of the radiation (Tummala
Rao, 2001). Similarly, a high relative permittivity (the real part
and not the imaginary part of a complex function describing it) provides an antithetical
effect. Hence, in general, a good capacitance, absorption, energy storage and high
loss of energy of radiation are found in high dielectric constant materials with a
high relative permittivity. |