Consider an RC circuit with a DC voltage supply as shown in the figure. There are four identical resistors (R=1.00 mega \mathrm{\Omega}) connected to one capacitor (C= 1.00 micro F). The voltage of the power supply is 10\times10^6 V. If the capacitor is fully charged and then the power supply is removed, find the current at t=0.5 s.
Answer:
All the four resistors are connected in parallel. The equivalent resistance of multiple parallel resistors is given by
\frac{1}{R_{\mathrm{eq}}}=\frac{1}{R_{\mathrm{1}}}+\frac{1}{R_{\mathrm{2}}}+\frac{1}{R_{\mathrm{3}}}+\cdots
In this case, we obtain
\frac{1}{R_{\mathrm{eq}}}=\frac{1}{R}+\frac{1}{R}+\frac{1}{R}+\frac{1}{R}=\frac{4}{R}
Thus,
R_{\mathrm{eq}}=\frac{R}{4}=\frac{1.00\times 10^6}{4}=2.50\times 10^5 \mathrm{\Omega}
From Kirchoff’s law, each circuit element consumes the voltage, and the total of it and supplied voltage must be zero. The capacitor consumes voltage, \frac{Q}{C} where Q is the total charge. The resistor consumes RI because of Ohm’s law. Since we consider the discharging process, voltage from the power supply is zero. Then, we have
-RI-\frac{Q}{C}=0
We know I=\frac{dQ}{dt}, so
\frac{dQ}{dt}+\frac{Q}{RC}=0
Solve this differential equation:
Q=Q_0 e^{-\frac{t}{RC}}
The charges and current flow are equivalent in terms of time, so can express it as
I=I_0 e^{-\frac{t}{RC}}
RC is known as the time constant, \tau=2.50\times 10^5 \times 1.00 \times 10^{-6}=0.25 s. I_0 is the current right before the voltage source is removed; namely, the maximum current. It can be calculated by Ohm’s law.
I_0=\frac{V}{R}=\frac{10\times 10^6}{2.50\times 10^5}=40.0 \ \mathrm{A}
Then, we can find the current at t=0.5 s.
I=40.0 e^{-\frac{0.5}{0.25}}=5.41 \ \mathrm{A}