Classical Electrodynamics |
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Page 13
Equations (1.13) and (1.16) can be combined into one partial differential
equation for the single function p(x): V*q = —4mp (1.28) This equation is called
Poisson's equation. In regions of space where there is no charge density, the
scalar ...
Equations (1.13) and (1.16) can be combined into one partial differential
equation for the single function p(x): V*q = —4mp (1.28) This equation is called
Poisson's equation. In regions of space where there is no charge density, the
scalar ...
Page 54
Spherical and cylindrical geometries are first considered, and solutions of
Laplace's equation are represented by ... Only an outline is given of the solution
of the various ordinary differential equations obtained from Laplace's equation by
...
Spherical and cylindrical geometries are first considered, and solutions of
Laplace's equation are represented by ... Only an outline is given of the solution
of the various ordinary differential equations obtained from Laplace's equation by
...
Page 582
The equation can be criticized on the grounds that it is second order in time,
rather than first, and therefore runs counter to the well-known requirements for a
dynamical equation of motion. This difficulty manifests itself immediately in the ...
The equation can be criticized on the grounds that it is second order in time,
rather than first, and therefore runs counter to the well-known requirements for a
dynamical equation of motion. This difficulty manifests itself immediately in the ...
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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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Common terms and phrases
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 |