Classical Electrodynamics |
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Page 392
For neutral particles with no detectable electromagnetic interactions it is clearly
impossible to obtain their relativistic transformation properties in this ... A charged
particle can be thought of as a very localized distribution of charge and mass.
For neutral particles with no detectable electromagnetic interactions it is clearly
impossible to obtain their relativistic transformation properties in this ... A charged
particle can be thought of as a very localized distribution of charge and mass.
Page 407
Since (p → p) = —mo, we see that for a free particle y L, is a constant, yL, - – A (
12.72) Then the action is proportional to the integral of the proper time over the
path from the initial space-time point a to the final space-time point b. This
integral ...
Since (p → p) = —mo, we see that for a free particle y L, is a constant, yL, - – A (
12.72) Then the action is proportional to the integral of the proper time over the
path from the initial space-time point a to the final space-time point b. This
integral ...
Page 443
13.4 Density Effect in Collision Energy Loss For particles which are not too
relativistic the observed energy loss is given accurately ... We have assumed that
it is legitimate to calculate the effect of the incident particle's fields on one
electron in ...
13.4 Density Effect in Collision Energy Loss For particles which are not too
relativistic the observed energy loss is given accurately ... We have assumed that
it is legitimate to calculate the effect of the incident particle's fields on one
electron in ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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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