Classical ElectrodynamicsProblems after each chapter |
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Page 130
... constant e ) , as shown in the figure . ( a ) Find the electric field everywhere between the spheres . ( b ) Calculate the surface - charge distribution on the inner sphere . ( c ) Calculate the polarization - charge density induced on ...
... constant e ) , as shown in the figure . ( a ) Find the electric field everywhere between the spheres . ( b ) Calculate the surface - charge distribution on the inner sphere . ( c ) Calculate the polarization - charge density induced on ...
Page 503
... constant and q / A = constant , no radiation is emitted by the system and the electric and magnetic fields of the system are the usual static values . ∞ , ( Note that for a real circuit the stationary positive ions in the conductors ...
... constant and q / A = constant , no radiation is emitted by the system and the electric and magnetic fields of the system are the usual static values . ∞ , ( Note that for a real circuit the stationary positive ions in the conductors ...
Page 614
... constant which is a universal constant perhaps having dimensions such that the electric field is dimensionally different from force per unit charge , There is , however , nothing to be gained by this extra freedom in the definition of E ...
... constant which is a universal constant perhaps having dimensions such that the electric field is dimensionally different from force per unit charge , There is , however , nothing to be gained by this extra freedom in the definition of E ...
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