Classical Electrodynamics |
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Page 10
(1.23) s |x — x"| Another problem of interest is the potential due to a dipole-layer
distribution on a surface S. A dipole layer can be imagined as being formed by
letting the surface S have a surface-charge density of X) on it, and another
surface ...
(1.23) s |x — x"| Another problem of interest is the potential due to a dipole-layer
distribution on a surface S. A dipole layer can be imagined as being formed by
letting the surface S have a surface-charge density of X) on it, and another
surface ...
Page 274
Considering only the magnetization term, we have the vector potential, - eikr 1 A(
x) = ik(n x m) —l 1 — -- (9.33) r ikr where m is the magnetic dipole moment, m-
size. -4s. x J) dor (9.34) C The fields can be determined by noting that the vector ...
Considering only the magnetization term, we have the vector potential, - eikr 1 A(
x) = ik(n x m) —l 1 — -- (9.33) r ikr where m is the magnetic dipole moment, m-
size. -4s. x J) dor (9.34) C The fields can be determined by noting that the vector ...
Page 628
... see Time dilatation Dimensions, discussion of, 611 Dipole approximation, in
energy loss, 435 in radiation problems, 271, 274, 507 Dipole fields, electrostatic,
100 magnetostatic, 143, 147 of conducting sphere, 34 of dielectric sphere, 115 of
...
... see Time dilatation Dimensions, discussion of, 611 Dipole approximation, in
energy loss, 435 in radiation problems, 271, 274, 507 Dipole fields, electrostatic,
100 magnetostatic, 143, 147 of conducting sphere, 34 of dielectric sphere, 115 of
...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
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