Classical ElectrodynamicsProblems after each chapter |
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Page 576
... ( defined in terms of the real part of the frequency ) in units of the radius a and the decay time ( defined as the time taken for the energy to fall to e1 of its initial value ) in units of the transit time ( a / c ) for each of the ...
... ( defined in terms of the real part of the frequency ) in units of the radius a and the decay time ( defined as the time taken for the energy to fall to e1 of its initial value ) in units of the transit time ( a / c ) for each of the ...
Page 614
... definition of E , since E is the first derived field quantity to be defined . Only when we define other field quantities may it be convenient to insert dimensional proportionality constants in the definitions in order to adjust the ...
... definition of E , since E is the first derived field quantity to be defined . Only when we define other field quantities may it be convenient to insert dimensional proportionality constants in the definitions in order to adjust the ...
Page 633
... definition of , 132 , 134 of circular loop , 141 of current element , 134 of long wire , 135 of magnetized sphere , 156 of nonrelativistic moving charge , 134 relativistic transformation of , 380 unit of , defined in terms of force ...
... definition of , 132 , 134 of circular loop , 141 of current element , 134 of long wire , 135 of magnetized sphere , 156 of nonrelativistic moving charge , 134 relativistic transformation of , 380 unit of , defined in terms of force ...
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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