An ideal resistor and an ideal inductor are joined in series across a sinusoidal…

PHYSICS · Multi-part · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Electromagnetic induction and alternating-current circuits · Electromagnetic induction and alternating-current circuits

Electricity, Magnetism and Electromagnetism, Ch AC circuits: phasors, complex impedance, resonance and power

Problem

An ideal resistor and an ideal inductor are joined in series across a sinusoidal source of angular frequency ω\omega. The connecting wires have zero resistance, and the source has been running long enough that only the steady sinusoidal response remains. In that steady state the current amplitude is 50 mA50\,\mathrm{mA}, the voltage across the resistor is vR=5.0cos⁡ωt Vv_R = 5.0\cos\omega t\ \mathrm{V} and the voltage across the inductor is vL=12cos⁡(ωt+90∘) Vv_L = 12\cos(\omega t + 90^\circ)\ \mathrm{V}. All phases are measured against cos⁡ωt\cos\omega t. ((a)) Add the two element voltages as phasors and write the source voltage in the form V0cos⁡(ωt+ϕ)V_0\cos(\omega t + \phi): give V0V_0 and ϕ\phi. ((b)) Find the magnitude ∣Z∣|Z| of the total impedance of the series pair.

Browse the problem library