Electricity and MagnetismA text for the standard electro-magnetism course for students in physics and engineering. Treats requisite theory with extensive examples of real-world applications. Offers coverage of topics neglected in most texts at this level, such as macroscopic vs. microscopic properties of matter. Also features a shorter, more student-oriented presentaton of the material, larger problem sets, and thorough discussion of alternative solution methods. |
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Page 88
... field E62 . The second and the fourth terms are the result of the introduction of the sphere in the external field . The second is only present when the sphere has a net charge Q , whereas the fourth is a dipole field produced by a ...
... field E62 . The second and the fourth terms are the result of the introduction of the sphere in the external field . The second is only present when the sphere has a net charge Q , whereas the fourth is a dipole field produced by a ...
Page 152
... field inside the sphere [ Eq . ( 4.86 ) ] vanishes and the field outside the sphere , Eq . ( 4.87 ) , becomes E2 ( ɛ1 - > ∞ ) = E62 + ER3 p3 [ 2f cos 0 + Ô sin 0 ] These electric fields are exactly the same fields produced when a ...
... field inside the sphere [ Eq . ( 4.86 ) ] vanishes and the field outside the sphere , Eq . ( 4.87 ) , becomes E2 ( ɛ1 - > ∞ ) = E62 + ER3 p3 [ 2f cos 0 + Ô sin 0 ] These electric fields are exactly the same fields produced when a ...
Page 337
... field H along the z axis . produced , say , by atom k at the site of atom j . Comparing Eq . ( 10.29 ) with U ' -Hom2H ' gives H'k = 20 нов2 mkz = ( 10.30 ) With the ... field produced along the z 10.4 FERROMAGNETISM 337 The Molecular Field.
... field H along the z axis . produced , say , by atom k at the site of atom j . Comparing Eq . ( 10.29 ) with U ' -Hom2H ' gives H'k = 20 нов2 mkz = ( 10.30 ) With the ... field produced along the z 10.4 FERROMAGNETISM 337 The Molecular Field.
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angle applied assume atoms axis becomes boundary conditions calculated called capacitor charge density charge distribution circuit coefficients components conducting conductor Consider constant continuous coordinates cylinder defined dependence derived Determine dielectric difference dipole direction discussed distance distribution effect electric field electrostatic element energy equal equation Example exists expression external fact Figure flux follows force frequency function given gives hence implies incidence inductance inside integral interface length loop magnetic field material medium method moving normal observer obtain origin parallel placed plane plates point charge polarization potential problem produced properties radiation radius reflection region relation resistance respectively result satisfy scalar shown in Fig solution solved space sphere spherical Substituting surface surface charge transformation unit vector volume wave wire write zero