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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 Too much Unique , stable solution in one direction 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 much Cauchy Open ...
... solution Too much Unique , stable solution in one direction 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 much Cauchy Open ...
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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ