Classical Electrodynamics |
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Page 104
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 quantities are
concerned, it is legitimate to talk of static fields and charges.” Furthermore, the
averaging ...
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 quantities are
concerned, it is legitimate to talk of static fields and charges.” Furthermore, the
averaging ...
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 3 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 3 from E and B.
Page 321
With this expression (10.42) for po, (10.41) can be written as p(r) = 1 s". d (r”B*) dr
(10.43) 8tt J, r* dr - The average pressure inside the cylinder can be related to the
total current I and radius R without specifying the detailed radial behavior.
With this expression (10.42) for po, (10.41) can be written as p(r) = 1 s". d (r”B*) dr
(10.43) 8tt J, r* dr - The average pressure inside the cylinder can be related to the
total current I and radius R without specifying the detailed radial behavior.
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
16 other sections not shown
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