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 400
... circuit behaves as an analog computer for appropriate RC and steady - state conditions . 13.3.3 The RLC Loop We now ... circuit , but practically may be concentrated in special in- ductors made of wire coils . The resistance of these ...
... circuit behaves as an analog computer for appropriate RC and steady - state conditions . 13.3.3 The RLC Loop We now ... circuit , but practically may be concentrated in special in- ductors made of wire coils . The resistance of these ...
Page 404
... RLC circuit . ( a ) Sketch of the circuit . ( b ) Time behavior of the charge on the capacitor . current will be zero , and we shall assume that the capacitor had no charge . Thus , the initial conditions are that I ( 0 ) : = 0 , and q ...
... RLC circuit . ( a ) Sketch of the circuit . ( b ) Time behavior of the charge on the capacitor . current will be zero , and we shall assume that the capacitor had no charge . Thus , the initial conditions are that I ( 0 ) : = 0 , and q ...
Page 422
... circuit is Î = Vy = V Ye ̄i Y = yl We will now discuss some properties of the circuit using the details of y . Res- onance for a parallel RLC circuit as here discussed is not so unambiguously defined as for the series case . We have ...
... circuit is Î = Vy = V Ye ̄i Y = yl We will now discuss some properties of the circuit using the details of y . Res- onance for a parallel RLC circuit as here discussed is not so unambiguously defined as for the series case . We have ...
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