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 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