Classical Electrodynamics |
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Page 16
We want to show the uniqueness of the solution of Poisson's equation, V*(p = —
47p, inside a volume V subject to either Dirichlet or Neumann boundary
conditions on the closed bounding surface S. We suppose, to the contrary, that
there exist ...
We want to show the uniqueness of the solution of Poisson's equation, V*(p = —
47p, inside a volume V subject to either Dirichlet or Neumann boundary
conditions on the closed bounding surface S. We suppose, to the contrary, that
there exist ...
Page 236
Then, just as in the static case, there is no electric field inside the conductors. The
charges inside a perfect conductor are assumed to be so mobile that they move
instantly in response to changes in the fields, no matter how rapid, and always ...
Then, just as in the static case, there is no electric field inside the conductors. The
charges inside a perfect conductor are assumed to be so mobile that they move
instantly in response to changes in the fields, no matter how rapid, and always ...
Page 260
The axial propagation constant k must be the same inside and outside the
cylinder in order to satisfy boundary conditions at all points on the surface at all
times. In the usual way, inside the dielectric cylinder the transverse Laplacian of
the ...
The axial propagation constant k must be the same inside and outside the
cylinder in order to satisfy boundary conditions at all points on the surface at all
times. In the usual way, inside the dielectric cylinder the transverse Laplacian of
the ...
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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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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 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 |