Classical ElectrodynamicsProblems after each chapter |
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Page 31
... Sphere In the previous section we considered the problem of a point charge q near a grounded sphere and saw that a surface - charge density was induced on the sphere . This charge was of total amount q ' = aqly , and was distributed ...
... Sphere In the previous section we considered the problem of a point charge q near a grounded sphere and saw that a surface - charge density was induced on the sphere . This charge was of total amount q ' = aqly , and was distributed ...
Page 33
... sphere held at a fixed potential V. The potential is the same as for the charged sphere , except that the charge ( Qq ' ) at the center is replaced by a charge ( Va ) ... sphere at fixed potential, Conducting sphere in a uniform field,
... sphere held at a fixed potential V. The potential is the same as for the charged sphere , except that the charge ( Qq ' ) at the center is replaced by a charge ( Va ) ... sphere at fixed potential, Conducting sphere in a uniform field,
Page 39
... sphere of radius R with a total charge on it . The potential has the constant value Q / R inside the sphere and falls off inversely with distance away from the center for points outside the sphere . By a suitable choice of center of ...
... sphere of radius R with a total charge on it . The potential has the constant value Q / R inside the sphere and falls off inversely with distance away from the center for points outside the sphere . By a suitable choice of center of ...
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