Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 85
Page 67
... spherical coordi- nates can be written in terms of spherical harmonics and powers of r in a generalization of ( 3.33 ) : 00 2 • ( r , 0 , 4 ) = Σ Σ [ Aimr2 + Bimr ̄ ( l + 1 ) ] Yım ( 0 , 4 ) ( 3.61 ) 1 = 0 m = -1 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 ) : 00 2 • ( r , 0 , 4 ) = Σ Σ [ Aimr2 + Bimr ̄ ( l + 1 ) ] Yım ( 0 , 4 ) ( 3.61 ) 1 = 0 m = -1 If the potential is ...
Page
... 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
... Spherical Bessel functions , see Bessel functions Spherical coordinates , 54 delta function in , 79 Im ' 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 Im ' Laplace's equation in , 54 Spherical harmonics , Y 64 f . addition theorem for , 67 and angular momentum , 542 completeness ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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