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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 ' = -aq / y , 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 ' = -aq / y , 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 Q 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 Q 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 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