Physic Labs

Problem 2

An ideal constant source of emf E=12.0 VE=12.0\,\mathrm V is connected at t=0t=0 in series with a resistor R=200,OmegaR=200,Omega and capacitor C=50.0,μFC=50.0,\mu\mathrm F. The capacitor is initially uncharged, and the wires and switch are ideal. Let q(t)q(t) be the charge on the plate connected toward the positive source terminal, and let i(t)=dq/dti(t)=dq/dt be the charging current, for tge0tge0. (a) Find the time constant and functions q(t)q(t) and i(t)i(t). (b) Find when the capacitor voltage reaches 9090% of its final value and the current then. (c) Find the stored energy at that instant and the limiting charge and current as t\toinftyt\toinfty.
t90=−RCln⁡(0.10)=2.303×10−2 s,i(t90)=0.10E/R=6.00 mAt_{90}=-RC\ln(0.10)=2.303\times10^{-2}\,\mathrm s,\quad i(t_{90})=0.10E/R=6.00\,\mathrm{mA}
problems.proof.analysis

Since VC=q/C=E(1−e−t/RC)V_C=q/C=E(1-e^{-t/RC}), setting VC=0.90EV_C=0.90E gives e−t/RC=0.10e^{-t/RC}=0.10. The current is then 1010% of its initial value, not 9090%, because the resistor drop supplies the remaining source voltage.

problems.proof.pitfall. At 90% of the final capacitor voltage, the current is only 10% of its initial value.