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 8
... coordinates . where { p , o , z } are defined at the point where the displacement dr is made . Geo- metrically this ... coordinates , we have dx dy dy dz dz dx 1 ( 1.20 ) corresponding to the surfaces z = constant , x = constant , and y ...
... coordinates . where { p , o , z } are defined at the point where the displacement dr is made . Geo- metrically this ... coordinates , we have dx dy dy dz dz dx 1 ( 1.20 ) corresponding to the surfaces z = constant , x = constant , and y ...
Page 18
... coordinate system in which it is represented . We shall see , for example , that VA has a physical meaning and retains that meaning independent of the system of coordinates in which A is ex- pressed . Thus , we shall assume that V × A ...
... coordinate system in which it is represented . We shall see , for example , that VA has a physical meaning and retains that meaning independent of the system of coordinates in which A is ex- pressed . Thus , we shall assume that V × A ...
Page 570
... coordinate system , the coordinates of the point change to ( x1 , x2 , x3 ) . The transformation is called linear if the new coordinates are given by a linear combination of the old coordinates ; that is , 3 x1 = [ a1jxj j = 1 ( 17.38 ) ...
... coordinate system , the coordinates of the point change to ( x1 , x2 , x3 ) . The transformation is called linear if the new coordinates are given by a linear combination of the old coordinates ; that is , 3 x1 = [ a1jxj j = 1 ( 17.38 ) ...
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Common terms and phrases
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 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 P₂ 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