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Page 67
... spherical coordi- nates can be written in terms of spherical harmonics and powers of r in a generalization of ( 3.33 ) : ¤ ( r , 0 , 4 ) = £ ≥ [ A¿mr2 + Bimr ̄ ( 1 + 1 ) ] Yım ( 0 , $ ) Σ 1 = 0 m = -1 ( 3.61 ) If the potential is ...
... spherical coordi- nates can be written in terms of spherical harmonics and powers of r in a generalization of ( 3.33 ) : ¤ ( r , 0 , 4 ) = £ ≥ [ A¿mr2 + Bimr ̄ ( 1 + 1 ) ] Yım ( 0 , $ ) Σ 1 = 0 m = -1 ( 3.61 ) If the potential is ...
Page 538
... spherical waves . These vector spherical waves are convenient for electromagnetic boundary - value problems possessing spherical symmetry properties and for the discussion of multipole radiation from a localized source distribution . In ...
... spherical waves . These vector spherical waves are convenient for electromagnetic boundary - value problems possessing spherical symmetry properties and for the discussion of multipole radiation from a localized source distribution . In ...
Page 638
... Spherical Bessel functions , see Bessel functions Spherical coordinates , 54 delta function in , 79 lm , Laplace's equation in , 54 Spherical harmonics , Y , 64 f . addition theorem for , 67 and angular momentum , 542 completeness ...
... Spherical Bessel functions , see Bessel functions Spherical coordinates , 54 delta function in , 79 lm , Laplace's equation in , 54 Spherical harmonics , Y , 64 f . addition theorem for , 67 and angular momentum , 542 completeness ...
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