Classical Electrodynamics |
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Page 19
... in (1.42) vanishes and the solution is on da (144) on' - For Neumann boundary
conditions we must be more careful. ... fox) 0GN (x, x') = 0 for x' on S 0n' since that
makes the second term in the surface integral in (1.42) vanish, as desired.
... in (1.42) vanishes and the solution is on da (144) on' - For Neumann boundary
conditions we must be more careful. ... fox) 0GN (x, x') = 0 for x' on S 0n' since that
makes the second term in the surface integral in (1.42) vanish, as desired.
Page 282
(9.64) With this condition on p it can readily be seen that the integral in (9.63)
over the hemisphere S, vanishes inversely as the hemisphere radius as that
radius goes to infinity. Then we obtain the Kirchhoff integral for p(x) in region II: ...
(9.64) With this condition on p it can readily be seen that the integral in (9.63)
over the hemisphere S, vanishes inversely as the hemisphere radius as that
radius goes to infinity. Then we obtain the Kirchhoff integral for p(x) in region II: ...
Page 284
(GE)] doz (9.74) y From the expansion, V × V x A = V(V. A.) – W*A, it is evident
that the volume integral vanishes identically.* With the surface integral of the first
three terms in (9.72) identically zero, the remaining three terms give an
alternative ...
(GE)] doz (9.74) y From the expansion, V × V x A = V(V. A.) – W*A, it is evident
that the volume integral vanishes identically.* With the surface integral of the first
three terms in (9.72) identically zero, the remaining three terms give an
alternative ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
6 other sections not shown
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle 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 shown in Fig 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 |