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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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |