Classical Electrodynamics |
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Page 297
The dimensions of the hole are assumed to be very small compared to a
wavelength of the electromagnetic fields which are assumed to exist on one side
of the sheet. The problem is to calculate the diffracted fields on the other side of
the ...
The dimensions of the hole are assumed to be very small compared to a
wavelength of the electromagnetic fields which are assumed to exist on one side
of the sheet. The problem is to calculate the diffracted fields on the other side of
the ...
Page 392
Foo,. (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 ...
Foo,. (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 ...
Page 567
John David Jackson. use of the spherical wave expansion (16.22) of the Green's
function (e”/4m R). We let |x| – o on both sides of (16.22). Then we can put |x — x"
| cr' — n - x on the left-hand side, where n is a unit vector in the direction of x'.
John David Jackson. use of the spherical wave expansion (16.22) of the Green's
function (e”/4m R). We let |x| – o on both sides of (16.22). Then we can put |x — x"
| cr' — n - x on the left-hand side, where n is a unit vector in the direction of x'.
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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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