Classical ElectrodynamicsProblems after each chapter |
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Page 104
... average over them at that instant will yield the same result as an average at some later instant of time . Hence , as far as the averaged quantities are concerned , it is legitimate to talk of static fields and charges . * Furthermore ...
... average over them at that instant will yield the same result as an average at some later instant of time . Hence , as far as the averaged quantities are concerned , it is legitimate to talk of static fields and charges . * Furthermore ...
Page 108
... average charge , and ( p , ) is their average dipole moment . Pex is the excess ( or free ) charge density . Usually the molecules are neutral , and the total charge density p is just the free charge density . With the definitions of ...
... average charge , and ( p , ) is their average dipole moment . Pex is the excess ( or free ) charge density . Usually the molecules are neutral , and the total charge density p is just the free charge density . With the definitions of ...
Page 197
... average . This is not the average of Poynting's theorem for microscopic fields , but differs from it by a set of terms which are the statement of energy conservation for the fluctuating fields measuring the instantaneous departure of ...
... average . This is not the average of Poynting's theorem for microscopic fields , but differs from it by a set of terms which are the statement of energy conservation for the fluctuating fields measuring the instantaneous departure 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