Classical Electrodynamics |
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Page 174
For such time-varying fields there are induced electromotive forces which cause
the sources of current to do work. Since the energy in the field is by definition the
total work done to establish it, we must consider these contributions. Suppose for
...
For such time-varying fields there are induced electromotive forces which cause
the sources of current to do work. Since the energy in the field is by definition the
total work done to establish it, we must consider these contributions. Suppose for
...
Page 208
Either o or k can be viewed as the independent variable when one considers
making a linear superposition. ... To allow for the possibility of dispersion we will
consider o as a general function of k: a) = 0(k) (7.25) Since the dispersive
properties ...
Either o or k can be viewed as the independent variable when one considers
making a linear superposition. ... To allow for the possibility of dispersion we will
consider o as a general function of k: a) = 0(k) (7.25) Since the dispersive
properties ...
Page 299
We will consider the scattering of a plane electromagnetic wave by a perfectly
conducting obstacle whose dimensions are large compared to a wavelength. For
a thin, flat obstacle, the techniques of Section 9.8, perhaps with Babinet's
principle, ...
We will consider the scattering of a plane electromagnetic wave by a perfectly
conducting obstacle whose dimensions are large compared to a wavelength. For
a thin, flat obstacle, the techniques of Section 9.8, perhaps with Babinet's
principle, ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
BoundaryValue Problems in Electrostatics II | 54 |
Copyright | |
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