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 ( Q — q ' ) at the center is replaced ... 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 ( Q — q ' ) at the center is replaced ... 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 / ) 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 / ) a and that the surface - charge density on an isolated disc raised to a given potential is proportional to ( a2 ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ