Classical ElectrodynamicsProblems after each chapter |
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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 91
... problem and variations of it have received considerable attention over the years . H. Weber ( 1873 ) first solved the present problem by using certain discontinuous integrals involving Bessel functions . Titchmarsh , p . 334 , uses ...
... problem and variations of it have received considerable attention over the years . H. Weber ( 1873 ) first solved the present problem by using certain discontinuous integrals involving Bessel functions . Titchmarsh , p . 334 , uses ...
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