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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 = a3Eo ( 4.62 ) oriented in ...
... 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 = a3Eo ( 4.62 ) oriented in ...
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 ...
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... 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 3 m2c3 2,2 dt 2 ( 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 3 m2c3 2,2 dt 2 ( 14.47 ) When this ...
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Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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