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Page 117
... seen as follows . Suppose that inside the sphere we have a cubic array of dipoles such as are shown in Fig . 4.12 , with all their moments constant in magnitude and oriented along the same direction ( remember that the sphere is ...
... seen as follows . Suppose that inside the sphere we have a cubic array of dipoles such as are shown in Fig . 4.12 , with all their moments constant in magnitude and oriented along the same direction ( remember that the sphere is ...
Page 155
... shown in Fig . 5.9 , Gauss's theorem can be applied to V. B = 0 to yield — ( B2 B1 ) n = 0 ( 5.88 ) where n is the unit normal to the surface directed from region 1 into region 2 , and the subscripts refer to values at the surface in ...
... shown in Fig . 5.9 , Gauss's theorem can be applied to V. B = 0 to yield — ( B2 B1 ) n = 0 ( 5.88 ) where n is the unit normal to the surface directed from region 1 into region 2 , and the subscripts refer to values at the surface in ...
Page 327
... described . The first is the kink instability , shown in Fig . 10.8a . The lines of azimu- thal magnetic induction near the column are bunched together above , and separated below , the column by the distortion downwards . Thus the ...
... described . The first is the kink instability , shown in Fig . 10.8a . The lines of azimu- thal magnetic induction near the column are bunched together above , and separated below , the column by the distortion downwards . Thus the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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