Classical Electrodynamics |
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Page 91
From (3.170) and an identity of Problem 3.12c this requirement can be seen to
imply lim f(k) = q (3.172) k->0 When boundary conditions (3.171) are applied to
the general solution (3.170), there results a pair of integral equations of the first ...
From (3.170) and an identity of Problem 3.12c this requirement can be seen to
imply lim f(k) = q (3.172) k->0 When boundary conditions (3.171) are applied to
the general solution (3.170), there results a pair of integral equations of the first ...
Page 284
To do this we make use of the following easily proved identities connecting
surface integrals over a closed surface S to volume ... (GE)] doz (9.74) y From the
expansion, V × V x A = V(V. A.) – W*A, it is evident that the volume integral
vanishes ...
To do this we make use of the following easily proved identities connecting
surface integrals over a closed surface S to volume ... (GE)] doz (9.74) y From the
expansion, V × V x A = V(V. A.) – W*A, it is evident that the volume integral
vanishes ...
Page 301
We see that Fon and Fm are proportional to (k+ kg), respectively; the shadow
integral will be large and the integral from the illuminated region will go to zero.
As the scattering angle departs from the forward direction the shadow integral will
...
We see that Fon and Fm are proportional to (k+ kg), respectively; the shadow
integral will be large and the integral from the illuminated region will go to zero.
As the scattering angle departs from the forward direction the shadow integral will
...
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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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