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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.
... 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.
Page 176
... electrostatic energy is expressed in terms of charge density and potential , can be obtained from ( 6.12 ) by assuming a linear relation between J and A. Then we find the magnetic energy to be 1 - √ W = 2c J.A d3x ( 6.17 ) The magnetic ...
... electrostatic energy is expressed in terms of charge density and potential , can be obtained from ( 6.12 ) by assuming a linear relation between J and A. Then we find the magnetic energy to be 1 - √ W = 2c J.A d3x ( 6.17 ) The magnetic ...
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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ