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Page 61
... coefficients A , are : 21 + 1 [ A1 ! [ * v ( 0 ) P , ( cos 6 ) sin 0 do = 2a1 I've ( 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 , 2 ...
... coefficients A , are : 21 + 1 [ A1 ! [ * v ( 0 ) P , ( cos 6 ) sin 0 do = 2a1 I've ( 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 , 2 ...
Page 370
... coefficients a , are constants characteristic of the particular transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients анг to satisfy the orthogonality condition : 4 Σαμναμ = μ = 1 бол With ( 11.71 ) it ...
... coefficients a , are constants characteristic of the particular transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients анг to satisfy the orthogonality condition : 4 Σαμναμ = μ = 1 бол With ( 11.71 ) it ...
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... 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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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 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