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 382
This magnetic field becomes almost equal to the transverse electric field E, as B
— 1. Even at nonrelativistic velocities where y o 1, this magnetic induction is
equivalent to B ~4 V × { (11.119) c ro which is just the Ampère-Biot–Savart ...
This magnetic field becomes almost equal to the transverse electric field E, as B
— 1. Even at nonrelativistic velocities where y o 1, this magnetic induction is
equivalent to B ~4 V × { (11.119) c ro which is just the Ampère-Biot–Savart ...
Page 597
It is desirable to have an equivalent equation of motion which is of the correct
order, has no grossly ... The smaller the particle's charge, the smaller the self-
fields, and the smaller the radiative effects, other things being equal. If the
external ...
It is desirable to have an equivalent equation of motion which is of the correct
order, has no grossly ... The smaller the particle's charge, the smaller the self-
fields, and the smaller the radiative effects, other things being equal. If the
external ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
16 other sections not shown
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