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
It can be considered as an equation which includes in some approximate and
time-average way the reactive effects of the emission of radiation. The equation
can be criticized on the grounds that it is second order in time, rather than first,
and ...
It can be considered as an equation which includes in some approximate and
time-average way the reactive effects of the emission of radiation. The equation
can be criticized on the grounds that it is second order in time, rather than first,
and ...
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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 |