An ignition coil of self-inductance has winding resistance and is connected through a…

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

Electricity, Magnetism and Electromagnetism, Ch Transients: RC, RL and LC circuits

Problem

An ignition coil of self-inductance L=8.0 mHL = 8.0\,\mathrm{mH} has winding resistance r=4.0 Ωr = 4.0\,\Omega and is connected through a switch to an ideal 12 V12\,\mathrm{V} battery (no internal resistance). A capacitor C=0.22 μFC = 0.22\,\mu\mathrm{F}, initially uncharged, is wired so that when the switch opens the coil's current is forced into it. All wires have zero resistance. ((a)) The switch is closed at t=0t = 0 with no current in the coil. From Kirchhoff's loop rule derive I(t)I(t), state the time constant and the final current, and evaluate II at t=1.0 mst = 1.0\,\mathrm{ms}. ((b)) Long afterwards the switch is opened, and the coil's current (which cannot jump) flows into the capacitor. For this fast stage the coil's resistance may be neglected, because the transient lasts tens of microseconds while L/rL/r is milliseconds. Show from the loop rule for the coil and capacitor that 12LI2+Q2/2C\tfrac12 LI^2 + Q^2/2C stays constant, and hence find the peak voltage reached across the capacitor. ((c)) After the transient the capacitor, holding that peak voltage, is left connected to a 100 kΩ100\,\mathrm{k}\Omega safety resistor. Derive its charge as a function of time from the loop rule, and find how long the capacitor voltage takes to fall to 1.0 V1.0\,\mathrm{V}.

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