Classical ElectrodynamicsProblems after each chapter |
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Page 33
... conducting 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 ... conducting sphere at fixed potential, Conducting sphere in a uniform field,
... conducting 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 ... conducting sphere at fixed potential, Conducting sphere in a uniform field,
Page 52
... conducting shell of radius a is in a uniform electric field E. If the sphere is cut into two hemispheres by a plane perpendicular to the field , find the force required to prevent the hemispheres from separa- ting ( a ) if the shell is ...
... conducting shell of radius a is in a uniform electric field E. If the sphere is cut into two hemispheres by a plane perpendicular to the field , find the force required to prevent the hemispheres from separa- ting ( a ) if the shell is ...
Page 53
... conducting sphere ? 2.10 Knowing that the capacitance of a thin , flat , circular , conducting disc of radius a is ( 2 / π ) a and that the surface - charge density on an isolated disc raised to a given potential is proportional to ( a2 ...
... conducting sphere ? 2.10 Knowing that the capacitance of a thin , flat , circular , conducting disc of radius a is ( 2 / π ) a and that the surface - charge density on an isolated disc raised to a given potential is proportional to ( a2 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ