Classical Electrodynamics |
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Page 20
Since the Green's function, as a function of one of its variables, is a potential due
to a unit point charge, this symmetry merely represents the physical
interchangeability of the source and the observation points. From form (1.40) for
G(x, x') it is ...
Since the Green's function, as a function of one of its variables, is a potential due
to a unit point charge, this symmetry merely represents the physical
interchangeability of the source and the observation points. From form (1.40) for
G(x, x') it is ...
Page 27
The original potential problem is on the left, the | equivalent-image problem on
the right. ... The image charges must be external to the volume of interest, since
their potentials must be solutions of Laplace's equation inside the volume; the ...
The original potential problem is on the left, the | equivalent-image problem on
the right. ... The image charges must be external to the volume of interest, since
their potentials must be solutions of Laplace's equation inside the volume; the ...
Page 94
(The segments are like the skin on wedges of an apple, or the earth's surface
between successive meridians of longitude.) The segments are kept at fixed
potentials + V, alternately. (a) Set up a series representation for the potential
inside the ...
(The segments are like the skin on wedges of an apple, or the earth's surface
between successive meridians of longitude.) The segments are kept at fixed
potentials + V, alternately. (a) Set up a series representation for the potential
inside 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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