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 119
... conductor does not permit the cavity field to penetrate the conductor . Therefore , the surface charge on the outer surface is " unaware " of the existence of the internal cavity . ( If there are no lines of force between two objects ...
... conductor does not permit the cavity field to penetrate the conductor . Therefore , the surface charge on the outer surface is " unaware " of the existence of the internal cavity . ( If there are no lines of force between two objects ...
Page 185
... conductor is given by = PQ where P is evaluated at the conductor . We will now prove the linearity of Eq . ( 6.9 ) in the case of two conductors . On the surface of the conductors , where the potentials are labeled 1 and 2 , we have ...
... conductor is given by = PQ where P is evaluated at the conductor . We will now prove the linearity of Eq . ( 6.9 ) in the case of two conductors . On the surface of the conductors , where the potentials are labeled 1 and 2 , we have ...
Page 189
... conductor . Clearly it gives the total amount of charge an isolated conductor can carry when at a poten- tial of 1 volt . It measures the " capacity " of a conductor to hold charge . As an application of Eq . ( 6.27 ) we determine the ...
... conductor . Clearly it gives the total amount of charge an isolated conductor can carry when at a poten- tial of 1 volt . It measures the " capacity " of a conductor to hold charge . As an application of Eq . ( 6.27 ) we determine 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