Classical ElectrodynamicsProblems after each chapter |
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Page 20
... physical interchangeability of the source and the observation points . From form ( 1.40 ) for G ( x , x ' ) it is clear that F ( x , x ' ) is also a symmetric function of its arguments . As a final , important remark we note the physical ...
... physical interchangeability of the source and the observation points . From form ( 1.40 ) for G ( x , x ' ) it is clear that F ( x , x ' ) is also a symmetric function of its arguments . As a final , important remark we note the physical ...
Page 190
... physical consequences . Hence it is customary to make the specific choice ( 6.83 ) . The physical meaning of the integral or differential form ( 6.81 ) or ( 6.82 ) is that the time rate of change of electromagnetic energy within a ...
... physical consequences . Hence it is customary to make the specific choice ( 6.83 ) . The physical meaning of the integral or differential form ( 6.81 ) or ( 6.82 ) is that the time rate of change of electromagnetic energy within a ...
Page 607
... physical requirements that ( a ) the normal modes of oscil- lation of the system must decay in time ( even if very slowly ) because of ever - present resistive losses , and ( b ) at high frequencies binding effects are unimportant and ...
... physical requirements that ( a ) the normal modes of oscil- lation of the system must decay in time ( even if very slowly ) because of ever - present resistive losses , and ( b ) at high frequencies binding effects are unimportant and ...
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Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ