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 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 ...
Page 95
3.5 3.6 3.7 3.8 3.9 A hollow sphere of inner radius a has the potential specified
on its surface to be p = V(0, b). Prove the equivalence of the two forms of solution
for the potential inside the sphere: _a(a” – ro V(0', 4') - (a) q}(x) = 4m. sa d() + a” ...
3.5 3.6 3.7 3.8 3.9 A hollow sphere of inner radius a has the potential specified
on its surface to be p = V(0, b). Prove the equivalence of the two forms of solution
for the potential inside the sphere: _a(a” – ro V(0', 4') - (a) q}(x) = 4m. sa d() + a” ...
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
Copyright | |
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