Classical ElectrodynamicsProblems after each chapter |
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Page 7
... position , and then to derive the vector quantities at the end if necessary ( see below ) . 1.5 Another Equation of Electrostatics and the Scalar Potential The single equation ( 1.13 ) is not enough to specify completely the three ...
... position , and then to derive the vector quantities at the end if necessary ( see below ) . 1.5 Another Equation of Electrostatics and the Scalar Potential The single equation ( 1.13 ) is not enough to specify completely the three ...
Page 124
... position . The initial electrostatic energy is = Wo = 1 8π JE E 。. Do d3x € 0 where Do E 。. Then with the sources fixed in position a dielectric object of volume V1 is introduced into the field , changing the field from E。 to E. The ...
... position . The initial electrostatic energy is = Wo = 1 8π JE E 。. Do d3x € 0 where Do E 。. Then with the sources fixed in position a dielectric object of volume V1 is introduced into the field , changing the field from E。 to E. The ...
Page 150
... position of lowest potential energy . We remark in passing that ( 5.73 ) is not the total energy of the magnetic moment in the external field . In bringing the dipole m into its final position in the field , work must be done to keep ...
... position of lowest potential energy . We remark in passing that ( 5.73 ) is not the total energy of the magnetic moment in the external field . In bringing the dipole m into its final position in the field , work must be done to keep ...
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