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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 x • B ) d3x ' + с ( 5.68 ) Use can now be made of identity ( 5.54 ) with the fixed ...
... 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 x • B ) d3x ' + с ( 5.68 ) Use can now be made of identity ( 5.54 ) with the fixed ...
Page 331
... depends on the sum of hydrostatic and magnetic pressures , apart from factors of the order of unity . If k is parallel to v4 , ( 10.72 ) reduces to ( k2v ̧2 — w2 ) ▽ 1 + A - 1 ) k2 ( V1 • V1 ) ▽ 1 = 0 V11 = 0 ( 10.74 ) ΝΑ = There are ...
... depends on the sum of hydrostatic and magnetic pressures , apart from factors of the order of unity . If k is parallel to v4 , ( 10.72 ) reduces to ( k2v ̧2 — w2 ) ▽ 1 + A - 1 ) k2 ( V1 • V1 ) ▽ 1 = 0 V11 = 0 ( 10.74 ) ΝΑ = There are ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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