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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 : дж φ ↓ ( $ 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 : дж φ ↓ ( $ 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 С ( E × H ) · n da + 1 E • 4πJ S ad at + H . . дв Ət d3x = - √ E · Jdz S ...
... 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 С ( E × H ) · n da + 1 E • 4πJ S ad at + H . . дв Ət d3x = - √ E · Jdz S ...
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