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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 W = 1 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 W = 1 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 approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ