Exercise E4 (Dis)Charging Capacities
(written test, approx. 14 % of a 60-minute written test, SS2023)
The circuit below has to be analyzed. The component values are:
- $U = 10 ~\rm V$
- $C_1 = 200 ~\rm nF$
- $R_1 = 8.0 ~\rm k\Omega$
- $R_2 = 17 ~\rm k\Omega$
- $R_3 = 7.0 ~\rm k\Omega$
- $I = 2.0 ~\rm mA$
Before $t_0$ all switches are switched as shown and the capacitor is fully discharged.
At $t_0=0 ~\rm s$ the switch $S_1$ shall switch to the voltage source.
1. Calculate the time constant for charging the capacitor.
Once $S_1$ is closed and $S_2$ is open at $t_0$, the source $U$ drives the current through the series circuit given by $S_1$, $C$, $R_1$ and $R_3$.
Therefore, $R= R_1 + R_3$
\begin{align*}
\tau_1 &= (R_1+R_3)\cdot C \\
&= (8~\rm k\Omega + 7~\rm k\Omega) \cdot 0.2 ~\rm \mu F \\
&= 15\cdot 10^{3} \cdot 0.2 \cdot 10^{-6} ~\rm {{V}\over{A}}{{As}\over{V}}\\
\end{align*}
2. What is the voltage $u_C$ at $t_1=t_0+4 ~\rm ms$?
3. The capacitors shall be charged to $U=10 ~\rm V$ at the time $t_2$.
At this point in time, the switch $S_1$ switches to the situation shown in the drawing.
What is the new time constant?
Now, $\rm S_1$ is opened and $\rm S_2$ is closed. Then, the source $U$ drives the current through the series circuit given by $\rm S_1$, $C$, $R_1$ and $R_2$.
Therefore, $R= R_1 + R_2$
\begin{align*}
\tau_2 &= (R_1+R_2)\cdot C \\
&= (8~\rm k\Omega + 17~\rm k\Omega) \cdot 0.2 ~\rm \mu F \\
&= 25\cdot 10^{3} \cdot 0.2 \cdot 10^{-6} ~\rm {{V}\over{A}}{{As}\over{V}}\\
\end{align*}
4. Draw the overall course of the voltage $u_C(t)$ over time in the diagram below.
Use an appropriate $x$-axis scale.
5. The switch $S_2$ is then closed, with $S_1$ still as shown in the drawing. What will be the maximum voltage of $u_C$?
The current of the source flows through the circuit consisting of $C$ in parallel with $R_1+R_2$. Without the parallel resistors, the current source would charge the capacitor „to infinity“ ($u_C \rightarrow \infty$) . This is here limited by the parallel resistors $R_1+R_2$.
The maximum voltage on the branch with the resisors $R_1+R_2$ is
\begin{align*} U_{12} &= R \cdot I \\ &= (R_1+R_2) \cdot I \end{align*}
This is also the maximum voltage on the capacitor, since it is in parallel with the resisors.
\begin{align*} U_C &= 50 ~\rm V \end{align*}