Classical Electrodynamics |
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Page 46
Then the expansion of an arbitrary function f($, m) is f(k, n) = 2, 2 a.m.U,(:)W,(m) (
2.44) where on on b d a--s assavow-oso (2.45) If the interval (a, b) becomes
infinite, the set of orthogonal functions U,($) may become a continuum of
functions, ...
Then the expansion of an arbitrary function f($, m) is f(k, n) = 2, 2 a.m.U,(:)W,(m) (
2.44) where on on b d a--s assavow-oso (2.45) If the interval (a, b) becomes
infinite, the set of orthogonal functions U,($) may become a continuum of
functions, ...
Page 148
... momentum, Li = M.(x: x v.). Thus (5.62) becomes - qi in -2Mc Li (5.63) If all the
particles in motion have the same charge to mass ratio (qis M. = e|M), the
magnetic moment can be written in terms of the total orbital angular momentum L:
...
... momentum, Li = M.(x: x v.). Thus (5.62) becomes - qi in -2Mc Li (5.63) If all the
particles in motion have the same charge to mass ratio (qis M. = e|M), the
magnetic moment can be written in terms of the total orbital angular momentum L:
...
Page 310
Then inertial effects enter and the conductivity becomes complex. Unfortunately
at these same frequencies the description of collisions in terms of a frictional
force tends to lose its validity. The whole process becomes more complicated.
Then inertial effects enter and the conductivity becomes complex. Unfortunately
at these same frequencies the description of collisions in terms of a frictional
force tends to lose its validity. The whole process becomes more complicated.
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
BoundaryValue Problems in Electrostatics II | 54 |
Copyright | |
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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 |
| Authors | John David Jackson, Patrick Thaddeus Jackson |
| Edition | 3 |
| Publisher | Wiley, 1962 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |