Classical Electrodynamics |
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Page 104
At any instant of time the very many charges in the volume AV will be in all
possible states of motion . An average over them at that instant will yield the
same result as an average at some later instant of time . Hence , as far as the
averaged ...
At any instant of time the very many charges in the volume AV will be in all
possible states of motion . An average over them at that instant will yield the
same result as an average at some later instant of time . Hence , as far as the
averaged ...
Page 108
+ pex where N, is the number of molecules of type i per unit volume, (e) is their
average charge, and (p,) is their average dipole moment. pes is the excess (or
free) charge density. Usually the molecules are neutral, and the total charge
density ...
+ pex where N, is the number of molecules of type i per unit volume, (e) is their
average charge, and (p,) is their average dipole moment. pes is the excess (or
free) charge density. Usually the molecules are neutral, and the total charge
density ...
Page 197
This is not the average of Poynting ' s theorem for microscopic fields , but differs
from it by a set of terms which are the statement of energy conservation for the
fluctuating fields measuring the instantaneous departure of e and ß from E and B
...
This is not the average of Poynting ' s theorem for microscopic fields , but differs
from it by a set of terms which are the statement of energy conservation for the
fluctuating fields measuring the instantaneous departure of e and ß from E and B
...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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