Classical Electrodynamics |
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Page 14
... Theorem If electrostatic problems always involved localized discrete or continuous distributions of charge with no boundary surfaces , the general solution ( 1.17 ) ... theorem : дф - ( ¿ V3y 14 Classical Electrodynamics Green's theorem,
... Theorem If electrostatic problems always involved localized discrete or continuous distributions of charge with no boundary surfaces , the general solution ( 1.17 ) ... theorem : дф - ( ¿ V3y 14 Classical Electrodynamics Green's theorem,
Page 25
... theorem : For charge - free space the value of the electrostatic potential at any point is equal to the average of the potential over the surface of any sphere centered on that point . 1.10 Use Gauss's theorem to prove that at the ...
... theorem : For charge - free space the value of the electrostatic potential at any point is equal to the average of the potential over the surface of any sphere centered on that point . 1.10 Use Gauss's theorem to prove that at the ...
Page 197
... theorem . We derived the conservation of energy in Section 6.8 in the macroscopic form ( 6.81 ) . Written out explicitly in terms of all the fields , it is · 4π Ꭻ Ꮪ √ ( Ex H ) · n da + ad дв E + H. 4π at ді -3B ) d x = √ E · J dz ...
... theorem . We derived the conservation of energy in Section 6.8 in the macroscopic form ( 6.81 ) . Written out explicitly in terms of all the fields , it is · 4π Ꭻ Ꮪ √ ( Ex H ) · n da + ad дв E + H. 4π at ді -3B ) d x = √ E · J dz ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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