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Page 104
... depends on the position of x , of the molecule , since the distortion of the charge cloud depends on the local field present . The microscopic electric field due to the jth * This ignores the very small ( at room temperature ) induction ...
... depends on the position of x , of the molecule , since the distortion of the charge cloud depends on the local field present . The microscopic electric field due to the jth * This ignores the very small ( at room temperature ) induction ...
Page 149
... depends on the fact that V x B = 0 for the external field , and that the gradient operator operates only on B. Then the force can be written F = — V · B ) d3x ' + с ( 5.68 ) Use can now be made of identity ( 5.54 ) with the fixed vector ...
... depends on the fact that V x B = 0 for the external field , and that the gradient operator operates only on B. Then the force can be written F = — V · B ) d3x ' + с ( 5.68 ) Use can now be made of identity ( 5.54 ) with the fixed vector ...
Page 331
... depends on the sum of hydrostatic and magnetic pressures , apart from factors of the order of unity . If k is parallel to v , ( 10.72 ) reduces to ( k2v ̧2 — w2 ) v1 + V1 ) V1 = 0 ( 10.74 ) = There are two types of wave motion possible ...
... depends on the sum of hydrostatic and magnetic pressures , apart from factors of the order of unity . If k is parallel to v , ( 10.72 ) reduces to ( k2v ̧2 — w2 ) v1 + V1 ) V1 = 0 ( 10.74 ) = There are two types of wave motion possible ...
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