Classical ElectromagnetismCLASSICAL ELECTROMAGNETISM features a friendly, informal writing style. The text has received numerous accolades. |
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Page 257
... inductor gets dissipated in the resistor . To find the time constant , we begin with V due to the inductor , SO dI V = - L and V = IR dt dI - L = IR dt The solution of the differential equation is The time constant I = Ioe - 1 / T T = L ...
... inductor gets dissipated in the resistor . To find the time constant , we begin with V due to the inductor , SO dI V = - L and V = IR dt dI - L = IR dt The solution of the differential equation is The time constant I = Ioe - 1 / T T = L ...
Page 323
... inductor carries 120 V × 0.32 A = 38 volt - amperes ( volt - amp is the unit of choice when the product does not represent watts of power dissipated ) ; so the inductor should be massive enough to handle a few watts . P < 0 Vr ( t ) I ...
... inductor carries 120 V × 0.32 A = 38 volt - amperes ( volt - amp is the unit of choice when the product does not represent watts of power dissipated ) ; so the inductor should be massive enough to handle a few watts . P < 0 Vr ( t ) I ...
Page 324
... inductor back into the AC outlet . One such region is marked in Figure 13.14 . So the average power is zero . And in fact our ideal inductor has no resistance ( nor hysteresis , Section 10.8 ) , so there is no way electrical energy can ...
... inductor back into the AC outlet . One such region is marked in Figure 13.14 . So the average power is zero . And in fact our ideal inductor has no resistance ( nor hysteresis , Section 10.8 ) , so there is no way electrical energy can ...
Contents
Vector Analysis | 1 |
Electric Field EGausss Law | 33 |
Magnetic Field BAmpères Law | 66 |
Copyright | |
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acceleration Ampère's law ANSWER antenna axis Biot-Savart Biot-Savart law calculate capacitance capacitor charge density charge Q circuit component conducting conductor constant coordinates Coulomb's law curl current density cylinder dielectric differential direction distance divergence E field electric dipole electric field electromagnetic electrons electrostatic energy example Faraday's law field lines Figure flux frequency Gauss's law inductance inductor infinite inside integral Laplace's equation line charge loop Lorentz force Lorentz transformation magnetic dipole magnetic field magnetic monopoles Maxwell's equations meter momentum moving negative parallel perpendicular plane plasma plates polarization positive potential Poynting's vector primed frame Problem radiation radius reference frame relative relativistic resistor right-hand rule scalar Section solenoid speed sphere spherical stationary surface charge theorem tion unit velocity voltage waveguide wire zero Απεργ Απερτ μο ду дх