Classical Electrodynamics |
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Page 46
Then the expansion of an arbitrary function f($, m) is f(k, n) = 2, 2 a.m.U.(5)W,(m) (
2.44) where b d sk + ann = | d5 | dou,"($)V,"(m)f($, m) (2.45) If the interval (a, b)
becomes infinite, the set of orthogonal functions U,($) may become a continuum ...
Then the expansion of an arbitrary function f($, m) is f(k, n) = 2, 2 a.m.U.(5)W,(m) (
2.44) where b d sk + ann = | d5 | dou,"($)V,"(m)f($, m) (2.45) If the interval (a, b)
becomes infinite, the set of orthogonal functions U,($) may become a continuum ...
Page 148
... position of the ith particle. Then the magnetic moment (5.55) becomes 1 in E. #
X*. x vi) (5.62) The vector product (x, x v.) is proportional to the ith particle's orbital
angular momentum, L = M.(x, x v.). Thus (5.62) becomes qi m = X —#1– L 5.63 ...
... position of the ith particle. Then the magnetic moment (5.55) becomes 1 in E. #
X*. x vi) (5.62) The vector product (x, x v.) is proportional to the ith particle's orbital
angular momentum, L = M.(x, x v.). Thus (5.62) becomes qi m = X —#1– L 5.63 ...
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 |
Nš 3 | 3 |
Greens theorem | 14 |
Copyright | |
30 other sections not shown
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Common terms and phrases
acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 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 result satisfy scalar scattering shows side simple 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 |