Classical ElectrodynamicsProblems after each chapter |
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Page 61
... coefficients A , are : Αι = 21 + 1 f 2a ' [ * v ( 0 ) P , V ( 0 ) P ( cos 0 ) sin 0 do d Ꮎ ( 3.35 ) If , for example , V ( 0 ) is that of Section 2.8 , with two hemispheres at equal and opposite potentials , + V , 0 ≤0 < V ( 0 ) = -V ...
... coefficients A , are : Αι = 21 + 1 f 2a ' [ * v ( 0 ) P , V ( 0 ) P ( cos 0 ) sin 0 do d Ꮎ ( 3.35 ) If , for example , V ( 0 ) is that of Section 2.8 , with two hemispheres at equal and opposite potentials , + V , 0 ≤0 < V ( 0 ) = -V ...
Page 372
... coefficients a ,, are constants characteristic of the particular transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients av to satisfy the orthogonality condition : 4 Σαμα Σα μ = 1 μλ = 812 With ( 11.71 ) ...
... coefficients a ,, are constants characteristic of the particular transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients av to satisfy the orthogonality condition : 4 Σαμα Σα μ = 1 μλ = 812 With ( 11.71 ) ...
Page 544
... coefficients Am in ( 16.35 ) are not completely arbitrary . The divergence condition V. B = 0 must be satisfied . Since the radial functions are linearly independent , the condition V. B = 0 must hold for the two sets of terms in ...
... coefficients Am in ( 16.35 ) are not completely arbitrary . The divergence condition V. B = 0 must be satisfied . Since the radial functions are linearly independent , the condition V. B = 0 must hold for the two sets of terms in ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ