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 16
... volume V of surface S into many infinitesimal volumes Av , of surfaces s , and the application of the definition of the divergence in terms of the infinitesimal volumes . for small Av . Consider a volume V with a surface S subdivided ...
... volume V of surface S into many infinitesimal volumes Av , of surfaces s , and the application of the definition of the divergence in terms of the infinitesimal volumes . for small Av . Consider a volume V with a surface S subdivided ...
Page 183
... volume over which p0 , or in fact any volume containing all the charge that has been assembled . If one has a continuously distributed charge , de- scribed by volume , surface , and line charge densities ( p , σ , and 2 ) , and point ...
... volume over which p0 , or in fact any volume containing all the charge that has been assembled . If one has a continuously distributed charge , de- scribed by volume , surface , and line charge densities ( p , σ , and 2 ) , and point ...
Page 278
... volume V and is nonzero only inside V. The vector potential is given by ( Eq . 8.42 ) , as follows : μο J ( r ' ) dv ' A ( r ) = 4π V ( 8.42 ) If ¿ = | r — r ' | is larger than the greatest linear dimension of V , we can expand the ...
... volume V and is nonzero only inside V. The vector potential is given by ( Eq . 8.42 ) , as follows : μο J ( r ' ) dv ' A ( r ) = 4π V ( 8.42 ) If ¿ = | r — r ' | is larger than the greatest linear dimension of V , we can expand the ...
Contents
VECTOR ANALYSIS | 1 |
ELECTROSTATICS | 28 |
ELECTROSTATIC BOUNDARY VALUE | 73 |
Copyright | |
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4περ A₁ Ampere's law angle atoms axis B₁ B₂ boundary conditions C₁ calculated capacitance capacitor charge density charge distribution charge q circuit coefficients components conducting conductor Consider constant coordinates current density cylinder dependence Determine dielectric displacement distance E₁ E₂ electric dipole electric field electromagnetic electron electrostatic element energy Example external ferromagnetic Figure flux force frequency function Gauss given by Eq gives H₂ hence inductance inside integral interface k₁ Laplace's equation linear loop Lorentz Lorentz transformation macroscopic magnetic field magnetic moment material Maxwell's equations medium molecules n₂ normal P₁ plane plates point charge polarization Poynting vector problem R₁ radiation radius region relation result RLC circuit scalar potential shown in Fig solenoid solution space sphere spherical surface charge transformation unit vector vector potential velocity voltage wire zero Απ Απερ μο