Classical ElectrodynamicsProblems after each chapter |
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Page 24
... conductors adjacent to each other . If equal and opposite charges are placed on the conductors , there will be a certain difference of potential between them . The ratio of the magnitude of the charge on one conductor to the magnitude ...
... conductors adjacent to each other . If equal and opposite charges are placed on the conductors , there will be a certain difference of potential between them . The ratio of the magnitude of the charge on one conductor to the magnitude ...
Page 236
... conductor on one side into a nonconducting medium on the other side . Then , just as in the static case , there is no electric field inside the conductors . The charges inside a perfect conductor are assumed to be so mobile that they ...
... conductor on one side into a nonconducting medium on the other side . Then , just as in the static case , there is no electric field inside the conductors . The charges inside a perfect conductor are assumed to be so mobile that they ...
Page 238
... conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written a n JE neglecting the other derivatives when operating on the fields within the conductor . With this approximation ( 8.5 ) ...
... conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written a n JE neglecting the other derivatives when operating on the fields within the conductor . With this approximation ( 8.5 ) ...
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