Classical ElectrodynamicsProblems after each chapter |
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Page 16
... solution is unique . Similarly , for Neumann boundary conditions , the solution is unique , apart from an unimportant arbitrary additive constant . From the right - hand side of ( 1.38 ) it is clear that there is also a unique solution ...
... solution is unique . Similarly , for Neumann boundary conditions , the solution is unique , apart from an unimportant arbitrary additive constant . From the right - hand side of ( 1.38 ) it is clear that there is also a unique solution ...
Page 17
... solution in one direction Closed surface Unique , stable solution Too much Too much Neumann Open surface Not enough Not enough Unique , stable solution in one direction Closed surface Unique , stable solution in Too much Too much ...
... solution in one direction Closed surface Unique , stable solution Too much Too much Neumann Open surface Not enough Not enough Unique , stable solution in one direction Closed surface Unique , stable solution in Too much Too much ...
Page 81
... solution , the general result ( 3.125 ) for a spherical shell is rather difficult to obtain by the method of images , since it involves an infinite set of images . 3.9 Solution of Potential Problems with the Spherical Green's Function ...
... solution , the general result ( 3.125 ) for a spherical shell is rather difficult to obtain by the method of images , since it involves an infinite set of images . 3.9 Solution of Potential Problems with the Spherical Green's Function ...
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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