Classical ElectrodynamicsProblems after each chapter |
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Page 189
... electromagnetic energy into mechanical or thermal energy . It must be balanced by a corresponding rate of decrease of energy in the electromagnetic field within the volume V. In order to exhibit this conservation law explicitly , we ...
... electromagnetic energy into mechanical or thermal energy . It must be balanced by a corresponding rate of decrease of energy in the electromagnetic field within the volume V. In order to exhibit this conservation law explicitly , we ...
Page 590
... electromagnetic structures of the neutron and proton . These have been explored by high - energy electron scattering , assuming that the electrons are point particles with no structure and that no changes occur in electro- dynamics at ...
... electromagnetic structures of the neutron and proton . These have been explored by high - energy electron scattering , assuming that the electrons are point particles with no structure and that no changes occur in electro- dynamics at ...
Page 621
... electromagnetic units in most common use today are the Gaussian and rationalized mks systems . The mks system has the virtue of overall convenience in practical , large - scale phenomena , especially in engineering applications . The ...
... electromagnetic units in most common use today are the Gaussian and rationalized mks systems . The mks system has the virtue of overall convenience in practical , large - scale phenomena , especially in engineering applications . The ...
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