Classical Electrodynamics |
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Page 25
... electrostatic energy and express it alternatively in terms of the equal and opposite charges Q and Q placed on the ... Electrostatics : I Many [ Probs . 1 ] 25 Introduction to Electrostatics 25.
... electrostatic energy and express it alternatively in terms of the equal and opposite charges Q and Q placed on the ... Electrostatics : I Many [ Probs . 1 ] 25 Introduction to Electrostatics 25.
Page 145
... electrostatic problem . Associated Legendre polynomials appear , as well as ordinary Legendre polynomials . This can be traced to the vector character of the current and vector potential , as opposed to the scalar properties of charge ...
... electrostatic problem . Associated Legendre polynomials appear , as well as ordinary Legendre polynomials . This can be traced to the vector character of the current and vector potential , as opposed to the scalar properties of charge ...
Page 634
... electrostatic , 98 electrostatic , expansion of interaction energy in , 101 electrostatic , expansion of potential in , 98 electrostatic , rectangular , 100 magnetostatic , 145 radiating , near , induction , and radia- tion zones , 270 ...
... electrostatic , 98 electrostatic , expansion of interaction energy in , 101 electrostatic , expansion of potential in , 98 electrostatic , rectangular , 100 magnetostatic , 145 radiating , near , induction , and radia- tion zones , 270 ...
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