AC Conductivity
Another way to incorporate attenuation is through the conductivity, as follows.
One of the equations governing electromagnetic wave propagation is the Maxwell-Ampere law:
- (SI) (cgs)
where D is the displacement field. Plugging in Ohm's law and the definition of (real) permittivity
- (SI) (cgs)
where is the (real, but frequency-dependent) conductivity, called AC conductivity. With sinusoidal time dependence on all quantities, i.e. and, the result is
- (SI) (cgs)
If the current J was not included explicitly (through Ohm's law), but only implicitly (through a complex permittivity), the quantity in parentheses would be simply the complex permittivity. Therefore,
- (SI) (cgs).
Comparing to the previous section, the AC conductivity satisfies
- (SI) (cgs).
Read more about this topic: Mathematical Descriptions Of Opacity