Classical Electrodynamics |
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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 general Too much Too ...
... 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 general Too much Too ...
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 ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ