Classical ElectrodynamicsProblems after each chapter |
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Page 11
... observation point by the area element da ' , as indicated in Fig . 1.7 . Note that d has a positive sign if 0 is an acute angle , i.e. , when the observation point views the " inner " side of the dipole layer . The potential can be ...
... observation point by the area element da ' , as indicated in Fig . 1.7 . Note that d has a positive sign if 0 is an acute angle , i.e. , when the observation point views the " inner " side of the dipole layer . The potential can be ...
Page 12
... observation point by the surface , regardless of its shape . There is a discontinuity of potential in crossing a double layer of an amount equal to 4 times the surface - dipole - moment density . This can be seen by letting the observation ...
... observation point by the surface , regardless of its shape . There is a discontinuity of potential in crossing a double layer of an amount equal to 4 times the surface - dipole - moment density . This can be seen by letting the observation ...
Page 292
... observation point from the diffracting system . Generally the diffracting system ( e.g. , an aperture in an opaque screen ) has dimensions comparable to , or large compared to , a wavelength . Then the observation point may be in the ...
... observation point from the diffracting system . Generally the diffracting system ( e.g. , an aperture in an opaque screen ) has dimensions comparable to , or large compared to , a wavelength . Then the observation point may be in the ...
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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