Classical ElectrodynamicsProblems after each chapter |
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Page 233
... Show that , except for sheets of very small thickness , the transmission coefficient is 32 ( Re ẞ ) 2e - 21 / 8 T ... Show that plane waves with frequency w and wave vector k must satisfy kx ( k × E ) + D = 0 = kn there are two distinct ...
... Show that , except for sheets of very small thickness , the transmission coefficient is 32 ( Re ẞ ) 2e - 21 / 8 T ... Show that plane waves with frequency w and wave vector k must satisfy kx ( k × E ) + D = 0 = kn there are two distinct ...
Page 369
... show that the invariant " length " element is ds2 = dx2 + dy2 + dz2 c2 dt2 - ( 11.60 ) This leads immediately to the ... shows that the time 7 , called the proper time of the particle , is a Lorentz invariant quantity . This is of ...
... show that the invariant " length " element is ds2 = dx2 + dy2 + dz2 c2 dt2 - ( 11.60 ) This leads immediately to the ... shows that the time 7 , called the proper time of the particle , is a Lorentz invariant quantity . This is of ...
Page 501
... Show that the instantaneous power radiated per unit solid angle is : e2c84 sin2 0 cos2 ( wt ' ) where ẞ = awo / c . dP ( t ' ) = ΦΩ 4πа2 ( 1 + ẞ cos 0 sin w。t ́ ) 5 ( b ) By performing a time averaging , show that the average power per ...
... Show that the instantaneous power radiated per unit solid angle is : e2c84 sin2 0 cos2 ( wt ' ) where ẞ = awo / c . dP ( t ' ) = ΦΩ 4πа2 ( 1 + ẞ cos 0 sin w。t ́ ) 5 ( b ) By performing a time averaging , show that the average power per ...
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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