Classical Electrodynamics |
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Page 24
Use symmetry arguments and Gauss's law to prove that (a) the surface-charge
densities on the adjacent faces are equal and opposite; (b) the surface-charge
densities on the outer faces of the two sheets are the same; (c) the magnitudes of
...
Use symmetry arguments and Gauss's law to prove that (a) the surface-charge
densities on the adjacent faces are equal and opposite; (b) the surface-charge
densities on the outer faces of the two sheets are the same; (c) the magnitudes of
...
Page 27
The original potential | problem is on the left, the | equivalent-image problem on
the right. ... It is clear that this is equivalent to the problem of the original charge
and an equal and opposite charge located at the mirror-image point behind the ...
The original potential | problem is on the left, the | equivalent-image problem on
the right. ... It is clear that this is equivalent to the problem of the original charge
and an equal and opposite charge located at the mirror-image point behind the ...
Page 382
This magnetic field becomes almost equal to the transverse electric field El as B
— 1. Even at nonrelativistic velocities where y c 1, this magnetic induction is
equivalent to B ~ 4 V × 5. - (11.119) c ro which is just the Ampère-Biot–Savart ...
This magnetic field becomes almost equal to the transverse electric field El as B
— 1. Even at nonrelativistic velocities where y c 1, this magnetic induction is
equivalent to B ~ 4 V × 5. - (11.119) c ro which is just the Ampère-Biot–Savart ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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