Classical Electrodynamics |
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Page 12
There is a discontinuity of potential in crossing a double layer of an amount equal
to 4t times the surface-dipole-moment density. This can be seen by letting the
observation point come infinitesimally close to the inner side of the double layer.
There is a discontinuity of potential in crossing a double layer of an amount equal
to 4t times the surface-dipole-moment density. This can be seen by letting the
observation point come infinitesimally close to the inner side of the double layer.
Page 292
Then the observation point may be in the near zone, less than a wavelength
away from the diffracting system. The near-zone fields are complicated in
structure and of little interest. Points many wavelengths away from the diffracting
system, but ...
Then the observation point may be in the near zone, less than a wavelength
away from the diffracting system. The near-zone fields are complicated in
structure and of little interest. Points many wavelengths away from the diffracting
system, but ...
Page 531
Then, in the dipole approximation, the appropriate intensity distribution is 4 0. 2 “”
-i. s n x ple” dt (15.80) 7T"C" IJ – od This gives 2 *; =#|esire (15.81) where 0 is the
angle between u and the observation direction n. In a semiclassical sense the ...
Then, in the dipole approximation, the appropriate intensity distribution is 4 0. 2 “”
-i. s n x ple” dt (15.80) 7T"C" IJ – od This gives 2 *; =#|esire (15.81) where 0 is the
angle between u and the observation direction n. In a semiclassical sense the ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
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