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 . -q 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 ...
... problem is on the left , the equivalent - image problem on the right . -q 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 ...
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 acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ