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Page xii
... expansion , 81 . 3.10 Expansion of Green's functions in cylindrical coordinates , 84 . 3.11 Eigenfunction expansions for Green's functions , 87 . 3.12 Mixed boundary conditions , charged conducting disc , 89 . References and suggested ...
... expansion , 81 . 3.10 Expansion of Green's functions in cylindrical coordinates , 84 . 3.11 Eigenfunction expansions for Green's functions , 87 . 3.12 Mixed boundary conditions , charged conducting disc , 89 . References and suggested ...
Page 44
... expansion parameter is ( a2 / x2 ) , rather than a2 , the series takes on the form : Φ ( α , θ , φ ) = 3Va2 2x2 - ( 5 12.c 8 3 32. " [ cos 0 - ( { 0 - 2 cos 0 ) + ··· ] α ( 2.33 ) For large values of x / a this expansion converges ...
... expansion parameter is ( a2 / x2 ) , rather than a2 , the series takes on the form : Φ ( α , θ , φ ) = 3Va2 2x2 - ( 5 12.c 8 3 32. " [ cos 0 - ( { 0 - 2 cos 0 ) + ··· ] α ( 2.33 ) For large values of x / a this expansion converges ...
Page 566
... expansion of a plane electromagnetic wave in spherical waves . For a scalar field y ( x ) satisfying the wave equation the necessary expansion can be obtained by using the orthogonality properties of the basic spherical solutions j ...
... expansion of a plane electromagnetic wave in spherical waves . For a scalar field y ( x ) satisfying the wave equation the necessary expansion can be obtained by using the orthogonality properties of the basic spherical solutions j ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ