Classical Electrodynamics |
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Page 392
Favo, (12.1) where v, = (v,ic), and F, is interpreted as the average field acting on
the particle. The left-hand side of (12.1) is now to be equated to the time rate of
change of the momentum and energy of the particle, just as in Section ...
Favo, (12.1) where v, = (v,ic), and F, is interpreted as the average field acting on
the particle. The left-hand side of (12.1) is now to be equated to the time rate of
change of the momentum and energy of the particle, just as in Section ...
Page 555
To determine the equation satisfied by the electric multipole function f,(r) inside
the source, we substitute (16.82) into the first equation of (16.80), take the scalar
product of both sides with a typical Xi, and integrate over all angles. All the terms
...
To determine the equation satisfied by the electric multipole function f,(r) inside
the source, we substitute (16.82) into the first equation of (16.80), take the scalar
product of both sides with a typical Xi, and integrate over all angles. All the terms
...
Page 567
We let |x"|→ oo on both sides of (16.22). Then we can put |x — x' co r" — n . x on
the left-hand side, where n is a unit vector in the direction of x'. On the right side r
= r" and r- = r. Furthermore we can use the asymptotic form (16.13) for h;”(kr').
We let |x"|→ oo on both sides of (16.22). Then we can put |x — x' co r" — n . x on
the left-hand side, where n is a unit vector in the direction of x'. On the right side r
= r" and r- = r. Furthermore we can use the asymptotic form (16.13) for h;”(kr').
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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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