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Page 45
... coefficients are given by an - 8 Un * ( 5 ) f ( $ ) d§ αξ ( 2.37 ) ( 2.38 ) where the orthonormality condition ( 2.35 ) has been used . This is the standard result for the coefficients in an orthonormal function expansion . If the ...
... coefficients are given by an - 8 Un * ( 5 ) f ( $ ) d§ αξ ( 2.37 ) ( 2.38 ) where the orthonormality condition ( 2.35 ) has been used . This is the standard result for the coefficients in an orthonormal function expansion . If the ...
Page 372
... coefficients a , are constants characteristic of the particular transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients a ,, to satisfy the orthogonality condition : Σαμναμλ = бил μ = 1 With ( 11.71 ) it ...
... coefficients a , are constants characteristic of the particular transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients a ,, to satisfy the orthogonality condition : Σαμναμλ = бил μ = 1 With ( 11.71 ) it ...
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 ▽ • 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 ▽ • B = 0 must hold for the two sets of terms in ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ