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Page 16
... problem . This is called a Dirichlet problem , or Dirichlet boundary conditions . Similarly it is plausible that specification of the electric field ( normal derivative of the potential ) every- where on the surface ( corresponding to a ...
... problem . This is called a Dirichlet problem , or Dirichlet boundary conditions . Similarly it is plausible that specification of the electric field ( normal derivative of the potential ) every- where on the surface ( corresponding to a ...
Page 27
... problem is on the left , the equivalent - image problem on the right . are called image charges , and the replacement of the actual problem with boundaries by an enlarged region with image charges but no boundaries is called the method ...
... problem is on the left , the equivalent - image problem on the right . are called image charges , and the replacement of the actual problem with boundaries by an enlarged region with image charges but no boundaries is called the method ...
Page 145
... problem and a cor- responding cylindrically symmetric electrostatic problem . Associated Legendre polynomials appear , as well as ordinary Legendre polynomials . This can be traced to the vector character of the current and vector ...
... problem and a cor- responding cylindrically symmetric electrostatic problem . Associated Legendre polynomials appear , as well as ordinary Legendre polynomials . This can be traced to the vector character of the current and vector ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ