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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 ) a3E 。 Eo ( 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 ) a3E 。 Eo ( 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 2 Peircular ( t ' ) = e2 3 m2c3 22 dt ( 14.47 ) When this is ...
... 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 2 Peircular ( t ' ) = e2 3 m2c3 22 dt ( 14.47 ) When this is ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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