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Page 115
... applied field with magnitude 3 Ein = Eo < Eo € + 2 ( 4.61 ) Outside the sphere the potential is equivalent to the applied field E plus the field of an electric dipole at the origin with dipole moment : - p = € + = ( = 1 ) a3 E。( 4.62 ) ...
... applied field with magnitude 3 Ein = Eo < Eo € + 2 ( 4.61 ) Outside the sphere the potential is equivalent to the applied field E plus the field of an electric dipole at the origin with dipole moment : - p = € + = ( = 1 ) a3 E。( 4.62 ) ...
Page 309
... applied to the solid conductor , but mass motion does not in general occur . The effects of the applied fields on the atoms themselves are taken up as stresses in the lattice structure . For a fluid , on the other hand , the fields act ...
... applied to the solid conductor , but mass motion does not in general occur . The effects of the applied fields on the atoms themselves are taken up as stresses in the lattice structure . For a fluid , on the other hand , the fields act ...
Page 475
... applied force . For circular motion , the magnitude of the rate of change of momentum ( which is equal to the applied force ) is ymv . Consequently , ( 14.46 ) can be written Peircular ( t ' ) = 2 e2 22 3 m2c3 dp dt ( 14.47 ) When this ...
... applied force . For circular motion , the magnitude of the rate of change of momentum ( which is equal to the applied force ) is ymv . Consequently , ( 14.46 ) can be written Peircular ( t ' ) = 2 e2 22 3 m2c3 dp dt ( 14.47 ) When this ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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