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 274
... loop da ' and the magnetic phenomena of small current loops at points distant from the loops ( thus the loops are small ) are indistinguishable from the magnetic phenomena of " magnetic dipoles . " 8.8.2 Magnetic Moments Even if a ...
... loop da ' and the magnetic phenomena of small current loops at points distant from the loops ( thus the loops are small ) are indistinguishable from the magnetic phenomena of " magnetic dipoles . " 8.8.2 Magnetic Moments Even if a ...
Page 364
... loop 1. It is as if we calculated the mutual inductances between the loop 1 and all the individual loops constituting the toroid , and then added them together . ( We neglect here the pitch of the toroid windings . ) Similarly , if we ...
... loop 1. It is as if we calculated the mutual inductances between the loop 1 and all the individual loops constituting the toroid , and then added them together . ( We neglect here the pitch of the toroid windings . ) Similarly , if we ...
Page 372
... loop of resistance R = 0.2 . The loop rotates about the z axis at ∞ = 2 × 500 rad / min ( keeping the same geometry ) , in a nonuniform magnetic field : B1 = 0.25μT at p1 and B2 = 0.8μT at p2 . ( a ) Determine the current in the loop ...
... loop of resistance R = 0.2 . The loop rotates about the z axis at ∞ = 2 × 500 rad / min ( keeping the same geometry ) , in a nonuniform magnetic field : B1 = 0.25μT at p1 and B2 = 0.8μT at p2 . ( a ) Determine the current in the loop ...
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