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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
... ( e ; ) is their average charge , and ( P :) is their average dipole moment . Pex is
the excess ( or free ) charge density . Usually the molecules are neutral , and the
total charge density p is just the free charge density . With the definitions of ( 4.36
) ...
... ( e ; ) is their average charge , and ( P :) is their average dipole moment . Pex is
the excess ( or free ) charge density . Usually the molecules are neutral , and the
total charge density p is just the free charge density . With the definitions of ( 4.36
) ...
Page 197
... like the statement of Poynting's theorem for the microscopic fields , except that
each quantity is replaced by its average . This is not the average of Poynting's
theorem for microscopic fields , but differs from it by a set of terms which are the ...
... like the statement of Poynting's theorem for the microscopic fields , except that
each quantity is replaced by its average . This is not the average of Poynting's
theorem for microscopic fields , but differs from it by a set of terms which are the ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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