Classical Electrodynamics |
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Page 193
Evidently the terms in the volume integral (6.93) transform like vectors. ... of
momentum, instead of the vectorial form (6.93), the tensor can be handled within
the framework of vector operations by introducing a corresponding dyadic. If a
tensor ...
Evidently the terms in the volume integral (6.93) transform like vectors. ... of
momentum, instead of the vectorial form (6.93), the tensor can be handled within
the framework of vector operations by introducing a corresponding dyadic. If a
tensor ...
Page 307
Make a sketch of I as a function of X for fixed Z. (c) Use the vector formula (9.82)
to obtain a result equivalent to that of part (a). Compare the two expressions. A
linearly polarized plane wave of amplitude Eo and wave number k is incident on
a ...
Make a sketch of I as a function of X for fixed Z. (c) Use the vector formula (9.82)
to obtain a result equivalent to that of part (a). Compare the two expressions. A
linearly polarized plane wave of amplitude Eo and wave number k is incident on
a ...
Page 640
Vector potential, for time-varying fields, 179 in magnetostatics, 139 f. in non-
cartesian coordinates, 141 of localized oscillating source, 269 f. of magnetic
dipole, 146 of oscillating electric dipole, 271 of oscillating electric quadrupole,
275 of ...
Vector potential, for time-varying fields, 179 in magnetostatics, 139 f. in non-
cartesian coordinates, 141 of localized oscillating source, 269 f. of magnetic
dipole, 146 of oscillating electric dipole, 271 of oscillating electric quadrupole,
275 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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