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Page 71
... Bessel functions of the first kind of order ± v . The series converge for all finite values of x . If v is not an integer , these two solutions J , ( x ) form a pair of linearly independent solutions to the second - order Bessel's ...
... Bessel functions of the first kind of order ± v . The series converge for all finite values of x . If v is not an integer , these two solutions J , ( x ) form a pair of linearly independent solutions to the second - order Bessel's ...
Page 74
... Bessel series and is particularly appropriate to functions which vanish at p = a ( e.g. , homogeneous Dirichlet boundary conditions on a cylinder ; see the following section ) . But it will be noted that an alternative expansion is ...
... Bessel series and is particularly appropriate to functions which vanish at p = a ( e.g. , homogeneous Dirichlet boundary conditions on a cylinder ; see the following section ) . But it will be noted that an alternative expansion is ...
Page 634
... functions , Bessel functions , 73 general , 44 Legendre polynomials , 57 spherical harmonics , 65 Orthogonality , of Bessel functions on finite interval , 73 , 95 of Bessel functions on infinite inter- val , 77 of Legendre polynomials ...
... functions , Bessel functions , 73 general , 44 Legendre polynomials , 57 spherical harmonics , 65 Orthogonality , of Bessel functions on finite interval , 73 , 95 of Bessel functions on infinite inter- val , 77 of Legendre polynomials ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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