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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 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ