Loading...

Here, a few sample AP Physics problems on circuits are gathered and solved. These questions involve the various configuration of capacitors, resistances, and electric power in a DC circuit.

**Problem (1): In the circuit below, find the equivalent resistance between points $A$ and $B$.**

**Solution**: One of the typical questions in all circuit practice problems is finding the equivalent resistance of a given circuit.

Recall that the equivalent of two resistors in series is $R_{eq}=R_1+R_2$ and in parallel is $\frac{1}{R_{eq}}=\frac{1}{R_1}+\frac{1}{R_2}$.

The two resistors $3-{\rm \Omega}$ are in series, so their equivalent resistance is \[R_{3,3}=R_3+R_3=3+3=6\,{\rm \Omega}\] It's obvious that resistors of $12\,{\rm \Omega}$ and $6\,{\rm \Omega}$ are in parallel, so their effective or equivalent resistance is \begin{align*}\frac{1}{R_{12,6}}&=\frac{1}{R_{12}}+\frac{1}{R_6}\\\\&=\frac{1}{12}+\frac{1}{6}=\frac{1+2}{12}\\\\\Rightarrow R_{12,6}&=4\quad{\rm \Omega}\end{align*} Now, $R_{12,6}$ is in series with the resistor of $8\,{\rm \Omega}$ which both have a effective resistance of \[R_{12,6,8}=R_{12,6}+R_8=4+8=12\,{\rm \Omega}\] In the end, we are left two resistance of $12\,{\rm \Omega}$ and $6\,{\rm \Omega}$ which are placed in parallel in the circuit (Because each are positioned on one side of points $A$ and $B$). Thus, the overall resistance of the circuit is determined as below \begin{align*}\frac{1}{R_{eq}}&=\frac{1}{R_{3,3}}+\frac{1}{R_{12,6,8}}\\\\&=\frac{1}{12}+\frac{1}{6}=\frac{1+2}{12}\\\\\Rightarrow R_{eq}&=4\quad{\rm \Omega}\end{align*}

Note: When two resistors $R_1$ and $R_2$ are in parallel, we can use the simple formula below to avoid using reciprocals \[R_{eq}=\frac{R_1 R_2}{R_1+R_2}\]

**Problem (2): The equivalent resistance between points $a$ and $b$ is $40\,{\rm \Omega}$ in the following electric circuit. If resistors $R$ are equal, find their value.**

**Solution**: The two resistances of $120\,{\rm \Omega}$ and $40\,{\rm \Omega}$ are in parallel, so we can remove these two resistors and replace them with their equivalent resistance which is \[R_{120,40}=\frac{R_1 R_2}{R_1+R_2}=\frac{120\times 40}{120+40}=30\,{\rm \Omega}\] Two resistors $5\,{\rm \Omega}$ and $R$ in the leftmost vertical branch are in series, so their equivalent resistance is $R_{R,5}=R+5$. These two latter equivalent resistances are also in parallel having an effective resistance of \[\frac{30\times (R+5)}{30+(R+5)}=\frac{30R+150}{R+35}\] In the end, this resistance is placed in series with the $R$ resistor. Thus, the overall resistance of the circuit is obtained as \[R_{eq}=R+\frac{30\times (R+5)}{30+(R+5)}\] Setting this $40\,{\rm \Omega}$ and Solving for $R$, we get the value of the unknown resistor \begin{gather*} R+\frac{30R+150}{R+35}=40 \\\\ \frac{R(R+35)+30R+150}{R+35}=40 \\\\ \Rightarrow 40R+1400=R^2+35R+30R+150 \\\\ \Rightarrow R^2+25R-1250=0 \end{gather*} To solve the quadratic equation $ax^2+bx^2+c=0$ where $a,b,c$ are some constants, use the following equation \[x=\frac{-b\pm\sqrt{b^2-4ac}}{2a}\] In this case, $a=1,b=25,c=-1250$, substituting these numerical values into the above equation, we obtain two solutions as \[R=\frac{2(1)\pm\sqrt{25^2-4(1)(-1250)}}{2(1)}\] The plus sign gives $\boxed{R=25\,{\rm \Omega}}$ and the minus sign gives $R=-50\,{\rm \Omega}$ which is incorrect (since the resistance can not be a negative value).

**Problem (3): In the following circuit, how much must $R_3$ be so that the equivalent resistance between $A$ and $B$ is $R_1$?**

**Solution**: Resistors $R_1$ and $R_2$ are in parallel, so their equivalent can be obtained by reciprocal-sum rule or the equation below \[R_{12}=\frac{R_1 \times R_2}{R_1+R_2}\] The result is a resistor which is in series with resistor $R_3$. Thus, the total equivalent resistance of the circuit is \[R_{eq}=R_{12}+R_3\] In the question it's told that the equivalent resistance of the circuit is $R_1$, so set $R_{eq}=R_1$ in the above equation, and solve for $R_1$. \begin{gather*} R_1 =\frac{R_1 \times R_2}{R_1+R_2}+R_3 \\\\ \Rightarrow R_3=R_1-\frac{R_1 \times R_2}{R_1+R_2}=\frac{R_1^2+R_1 R_2-R_1 R_2}{R_1+R_2} \\\\ \Longrightarrow \boxed{R_3=\frac{R_1^2}{R_1+R_2}}\end{gather*}

**Problem (4): In the circuit below, how much current passes through the $1.5-{\rm \Omega}$ resistor?**

**Solution**: In this kind of question, first of all, find the total equivalent resistance of the circuit, then using Ohm's law find the amount of total current delivered by the battery.

Two resistors $3\,{\rm \Omega}$ and $1.5\,{\rm \Omega}$ are in parallel, so their equivalent resistance is \[R_{eq}=\frac{3\times 1.5}{3+1.5}=1\,{\rm \Omega}\] This effective resistor is placed in series with the remaining external resistance of the circuit, $3.5\,{\rm \Omega}$. With this simplification, the circuit involves the resistances of $1\,{\rm \Omega}$, $3.5\,{\rm \Omega}$, and the internal resistance of the battery. Thus, combine them to find the total equivalent resistance of the circuit \[R_t=1+3.5=4.5\,{\rm \Omega}\]

All these resistors are in series with each other, so a common current flows through each. This current flow is the same current delivered by the buttery into the circuit. But how much current?

When a circuit is connected to a source of emf (battery), the total current through the battery is found by the following formula \[I_t=\frac{\mathcal{E}}{r+R_{eq}}=\frac{6}{1.5+4.5}=1\,{\rm A}\] Thus, through each resistor a current of $1\,{\rm A}$ flows. The next step is to find the current through the $1.5\,{\rm \Omega}$ resistor which is a part of $1\,{\rm \Omega}$ combined resistor.

The two $1.5\,{\rm \Omega}$ and $3\,{\rm \Omega}$ resistors are in parallel with each other. Recall that the voltages across resistors in parallel are the same i.e. $V_3=V_{1.5}$. Using this fact and Ohm's law, we find a relation between the current through these two resistors as below \begin{gather*} V_3=V_{1.5} \\\\ I_3 R_3=I_{1.5}R_{1.5}\\\\ 3I_3=1.5I_{1.5} \\\\ \Rightarrow \boxed{I_3=\frac 12 I_{1.5}}\end{gather*} The $1-{\rm A}$ total current provided by the battery when reaches the junction $a$, splits into the two currents $I_3$ and $I_{1.5}$. So, their sum must be the same total current (i.e., $I_t=I_3+I_{1.5}$).

In this case, we have $I_{1.5}+I_3=1\,{\rm A}$. Therefore, substituting the boxed relation above into this, we get \begin{gather*} I_{1.5}+\frac 12 I_{1.5}=1 \\\\ \Rightarrow (1.5)I_{1.5}=1 \\\\ \Rightarrow I_{1.5}=\frac{1}{1.5}=\frac 23 \,{\rm A}\end{gather*} Thus, the current through $1.5\,{\rm \Omega}$ is $1.5\,{\rm A}$.

*Further reading:
Ohm's law Practice problems with solutions*

**Problem (5): The $33-{\rm \Omega}$ resistor dissipates $0.8\,{\rm W}$ in the circuit shown below. Find the voltage across the battery.**

**Solution**: The battery voltage is unknown. By having the total current flowing from the battery and equivalent resistance of the circuit, using Ohm's law, $V_t=I_t R_t$, we can find the voltage across the battery.

The power dissipated by resistance is found by the following formulas \[P=R i^2=\frac{V^2}{R}=Vi\] where $V$ is the voltage across the resistance and $i$ is the current through it.

In this circuit the $33-{\rm \Omega}$ resistor is connected directly to the battery, so all the current delivered by the battery flows through it. In other words, the current passing through this resistor gives the total current of the circuit.

Using the power formula $P=R i^2$, and solving for $i$, we can find the current flowing from the $33-{\rm \Omega}$ resistor \[i=\sqrt{\frac{P}{R}}=\sqrt{\frac{0.8}{33}}=0.156\,{\rm A}\] This is the total current flowing from the battery $I_t=0.156\,{\rm A}$. Now we must find the equivalent resistance of the circuit.

The two resistors of $68\,{\rm \Omega}$ and $85\,{\rm \Omega}$ are in parallel, so their equivalent resistance is found as below \[R_{eq}=\frac{68\times 85}{68+85}=37.7\,{\rm \Omega}\] This new resistor is placed in series with the $33-{\rm \Omega}$ resistor, so the total equivalent resistance of the circuit is \[R_t=33+37.7=70.7\quad {\rm \Omega}\] Given the total current and resistance of the circuit, one can find the voltage across the battery using Ohm's law as below \[V_t=I_t R_t=0.15\times 70.7=11\,{\rm V}\]

**Problem (6): In the circuit shown below, the $2-{\rm \Omega}$ resistor dissipates a power of $18\,{\rm W}$ in the circuit. What is the voltage between points $A$ and $B$? **

**Solution**: The voltage between points $A$ and $B$ is the sum of voltages across $4-{\rm \Omega}$ resistor and the loop. \[V_{AB}=V_{cd}+V_{ef}\] Our task is to find these two unknown voltages.

The resistors $2-{\rm \Omega}$ and $6-{\rm \Omega}$ are in series, so the currents through them are the same. Given the power dissipated by $2-{\rm \Omega}$ resistor and using the power formula $P=Ri^2$, we can find the current flowing from this resistor \[i=\sqrt{\frac{P}{R}}=\sqrt{\frac{18}{2}}=3\,{\rm A}\] Thus, $I_2=I_4=3\,{\rm A}$. The equivalent resistance of these two is \[R_{2,6}=R_2+R_6=2+6=8\,{\rm \Omega}\] The total current and equivalent resistance of the upper branch are known, so using Ohm's law, we can find the voltage across this branch as \[V_{up}=IR=3\times 8=24\,{\rm V}\] The lower branch also has the same voltage as the up branch according to this rule that the voltages across parallel branches are the same. Therefore, \[V_{upper}=V_{lower}=V_{ef}=24\,{\rm V}\]

Given the voltage of the lower branch, one can find the current through the $12-{\rm \Omega}$ resistor. \[i_{12}=\frac{V}{R_{12}}=\frac{24}{12}=2\,{\rm A}\] The sum of currents flowing from the upper and lower branches (parallel branches) gives us the total current before splitting into those (junction rule in Kirchhoff's rule). Hence, \[i_{ef}=i_{upper}+i_{lower}=3+2=5\,{\rm A}\] This is the current flowing also from the $4-{\rm \Omega}$, since it is placed in series with the equivalent resistance between points $e$ and $f$ (find yourself $R_{ef}=?$).

Therefore, using Ohm's law the voltage $V_{cd}$ is calculated as \[V_{cd}=i_{cd}R_4=5\times 4=20\,{\rm V}\] Hence, the voltage across the points $A$ and $B$ is \[V_{AB}=V_{cd}+V_{ef}=20+24=44\,{\rm V}\]

**Problem (7): In the circuit shown below, the voltage drop across the internal resistance and the $2.5-{\rm \Omega}$ resistor are $0.25\,{\rm V}$ and $1.25\,{\rm V}$, respectively. Find the emf and internal resistance of the battery.**

**Solution**: The potential drop across the internal resistance of a battery is defined as $V_r=Ir$, and across the resistor external to the battery is $V_R=IR$ where $I$ is the total current through the circuit.

Using these two facts and their given numerical values, we can find the their ratio \begin{align*} \frac{V_r}{V_R}&=\frac{Ir}{IR}\\\\ \frac{0.25}{1.25}&=\frac{r}{2.5}\\\\ \Rightarrow r&=0.5\,{\rm \Omega}\end{align*} Thus, the internal resistance of the battery is $\boxed{r=0.5\,{\rm \Omega}}$.

In a simple circuit involving a source of emf with internal resistance $r$ and an external resistance $R$, the current delivered by the battery is found using the formula \[I=\frac{\mathcal E}{r+R}\] Rearranging this, and substituting the given values, we have \begin{align*} \mathcal{E}&=IR+Ir\\\\ &=V_R+V_r \\\\ &=1.25+0.25\\\\&=1.5\quad {\rm V}\end{align*} Thus, the emf of the battery is $\boxed{\mathcal{E}=1.5\,{\rm V}}$

**Problem (8): In the circuit below, when the switch is opened, the voltmeter shows $12\,{\rm V}$, and when it is closed, the voltmeter reading is $10\,{\rm V}$. What are the emf and the internal resistance of the battery? **

**Solution**: Remember that in a circuit including a source of emf with an internal resistance of $r$ and an equivalent resistance of $R_{eq}$ due to other resistances external to the battery, the total current flowing through the circuit is found by the formula below \[I=\frac{\mathcal{E}}{r+R_{eq}}\] Here, voltmeter is connected across the terminals of the battery, so it shows the battery's terminal voltage. Always, the terminal voltage is given by $\Delta V=\mathcal{E}-Ir$, where $I$ is the total current through the circuit.

In this circuit, when the switch $K$ is opened, there is no closed loop including the battery (except the loop with the voltmeter), so the current through the circuit is zero, $I=0$. Substituting this into the terminal voltage formula above, the emf of the battery is obtained \[V_{ab}=\mathcal{E}-Ir \Rightarrow V_{ab}=\mathcal{E}=12\,{\rm V}\] When the switch $K$ is closed, the two other external resistors come into play. These two resistors are in series with each other, so their equivalent resistance is the sum of each. \[R_{eq}=R_8+R_{12}=8+12=20\,{\rm \Omega}\] In this case, the terminal voltage or voltmeter reading is \[V_{ab}=\mathcal{E}-Ir \Rightarrow \boxed{10=12-Ir}\] $I$ is also found using the formula below \[I=\frac{\mathcal{E}}{r+R_{eq}}=\frac{12}{r+20}\] Substituting this into the above boxed equation, and solving for $r$, we have \begin{gather*} 10=12-\left(\frac{12}{r+20}\right)r \\\\ \frac{12r}{r+20}=12-10=2\\\\ 6r=r+20 \\\\ 5r=20 \\\\ \Rightarrow r=4\,{\rm \Omega}\end{gather*}

**Problem (9): What happens to the reading of the ammeter and voltmeter for the circuit below when the switch $S$ is closed?**

**Solution**: The ammeter reads the total current $I$ through from the battery or the circuit, whose value is found by \[I=\frac{\mathcal{E}}{r+R_{eq}}\] The voltmeter is also read the terminal voltage across the battery whose value is given by \[V_{ab}=\mathcal{E}-Ir\] where $r$ is the internal resistance of the battery.

When the switch is opened, the middle branch is removed from the circuit, so the equivalent resistance of the circuit equals $R_{eq}=R$. Correspondingly, the current in this case is \[I_O=\frac{\mathcal{E}}{r+R_{eq}}=\frac{\mathcal{E}}{r+R}\] where $I_O$ is the current when the switch is open. By opening the switch, the voltmeter reading is also found as \begin{align*} V_O&=\mathcal{E}-I_O r\\\\ &=\mathcal{E}-\left(\frac{\mathcal{E}}{r+R}\right)r \\\\&=\frac{\mathcal{E}R}{R+r}\end{align*} Now we turn to the case of closing the switch $S$. In this case, the equivalent resistance is \[R_{eq}=\frac{R\times R}{R+R}=\frac R2\] Since the resistors are in parallel. The ammeter shows the total current flowing from the battery whose value is \[I_C=\frac{\mathcal{E}}{r+R_{eq}}=\frac{\mathcal{E}}{r+R/2}\] On the other side, as mentioned, the voltmeter indicates the voltage across the battery or terminal voltage with the following value \begin{align*} V_C&=\mathcal{E}-I_C r\\\\ &=\mathcal{E}-\left(\frac{\mathcal{E}}{r+R/2}\right)r \\\\&=\frac{\mathcal{E}R}{R+2r}\end{align*} Now we compare the currents and voltages before and after closing the switch $K$: \begin{gather*} \frac{\mathcal{E}}{r+R/2}> \frac{\mathcal{E}}{r+R} \\\\ \Rightarrow \boxed{I_C > I_O} \\\\ \frac{\mathcal{E}R}{R+r} > \frac{\mathcal{E}R}{R+2r} \\\\\Rightarrow \boxed{V_O > V_C} \end{gather*}

**Problem (10): (a) Four $3.2-{\rm \mu F}$ capacitor are connected in series. What is the equivalent capacitance? (b) Assuming now they are connected in parallel, what is their equivalent capacitance? **

**Solution**: (a) When a number of capacitors are connected in series, say $C_1, C_2, C_3,\cdots$, their equivalent capacitance is given by the following formula \[\frac{1}{C_{eq}}=\frac{1}{C_1}+\frac{1}{C_2}+\frac{1}{C_3}+\cdots\] Therefore, in this case, the equivalent capacitance is \[\frac{1}{C_{eq}}=\frac{1}{3.2}+\frac{1}{3.2}+\frac{1}{3.2}+\frac{1}{3.2}=\frac{4}{3.2}\] By inverting, we have $C_{eq}=0.8\,{\rm \mu F}$.

(b) When those capacitors are in parallel, their equivalent capacitance becomes \[C_{eq}=C_1+C_2+C_3+\cdots\] Thus, in this case, the equivalent capacitance is \[C_{eq}=4(3.2)=12.8\,{\rm \mu F}\]

**Problem (11): In the following circuit, what is the potential difference across the capacitor?
a. 8V b. 10V c. 6V d. 15V**

**Solution**: As can be seen from the circuit, the two $4-{\rm \Omega}$ resistors are in parallel, so we compute their combined resistance and replace them with those. \[R_{eq}=\frac{R_1 R_2}{R_1+R_2}=\frac{4\times 4}{4+4}=2\,{\rm \Omega}\] Note that when a fully charged capacitor is present in an electric circuit, that branch acts as an open circuit, which means the current no longer flows through it. Because, in practice, the capacitor behaves like a resistor with infinite resistance.

On the other side, the current delivered by a source of emf (battery) with internal resistance $r$ and external resistance $R_{eq}$ is found by \[I=\frac{\mathcal{E}}{r+R_{eq}}=\frac{12}{1+2}=4\,{\rm A}\] All this current flows through the equivalent resistance of $2\,{\rm \Omega}$. Given that, we can find the potential drop across this combined resistor, using Ohm's law, as \[V=IR=4\times 2=8\,{\rm V}\] Now pay attention to this fact that the capacitor and $2-{\rm \Omega}$ equivalent resistance are in parallel which means the voltage across the capacitor is the same as the voltage across the resistor (i.e., $V_C=V_{2R}$).

Hence, the potential (voltage) difference across the capacitor is $\boxed{8\,{\rm V}}$.

**Problem (12): In the circuit diagram shown below, how much charge is on the plates of the capacitor stored? **

**Solution**: The charge stored on the plates of a capacitor is related to the voltage across it by $Q=C\Delta V$. The capacitance of the capacitor is known, the only thing that we must find is the potential drop (voltage) across it.

On the other side, you can see that the capacitor is connected in parallel with the $4-{\rm \Omega}$ resistor, which means that the voltage difference across the capacitor is the same as the resistor. So, our task is to find the voltage across the $4-{\rm \Omega}$ resistor, $\Delta V_4=IR$, which is subsequently needed to find the current through that resistor.

As a rule of thumb, *ignore that branch of the circuit that includes the capacitor since the capacitors in an electric circuit (when it is fully charged) act as a resistor with an infinite resistor and do open the circuit. *

With this long introduction, let's move on to solving the problem.

By ignoring the capacitor, the three $4-{\rm \Omega}$ resistors are in series with a equivalent resistance of $R_{eq}=3(4)=12\,{\rm \Omega}$. This new resistor is in parallel with the other $4-{\rm \Omega}$ resistor in the middle branch.

Thus, the total equivalent resistance of the circuit is \[R_t=\frac{R_1 R_2}{R_1+R_2}=\frac{4\times 12}{4+12}=3\,{\rm \Omega}\] The total current flowing through the circuit is \[I_t=\frac{\mathcal{E}}{r+R_t}=\frac{24}{0+3}=8\,{\rm A}\] This current splits into two parts: $I_1$, flowing through $abcd$ loop; and $I_2$, flowing through $ad$ branch (i.e., $I_t=I_1+I_2$). Since the $ad$ branch is in parallel with the battery, so the voltage across it is the same as the battery (i.e., $V_{ad}=24\,{\rm V}$). Given that, we can find the current, $I_2$ through it as \[I_2=\frac{V_{ad}}{R}=\frac{24}{4}=6\,{\rm A}\] So, the current $I_1$ is also found as \[I_t=I_1+I_2 \Rightarrow I_1=2\,{\rm A}\] All resistors in the $abcd$ branch are in series, so a common current (i.e., $I_1$) flowing through each of them. Using Ohm's law, $\Delta V=IR$, we can find the voltage across the resistance which is in parallel with the capacitor \[\Delta V_4=I_2 R_4 =2\times 4=8\,{\rm V}\] At the beginning, we argued that $\Delta V_4=\Delta V_C$, so the potential drop across the capacitor is $\Delta V_C=8\,{\rm V}$. Given that, using the definition of capacitance, $C=\frac{Q}{\Delta V}$, one can find the charge stored on the plates of the capacitor \begin{align*} Q&=C\Delta V=(5\times 10^{-6})(8) \\\\ &=40\times 10^{-6}\quad {\rm C} \\\\ &=40\quad {\rm \mu C}\end{align*}

**Problem (13): In the circuit shown below, the capacitor does not have any charge on its plates. Immediately after closing the switch $S$, what are the currents $I_1$ and $I_2$, respectively?
a. 1, 1 b. 1.5, 0 c. 0, 1.5 d. 1.5, 3**

**Solution**: When a capacitor is placed (no matter in parallel or series) with a resistor in a circuit, just after closing the switch, it acts as a wire without any resistance.

Conversely, after passing a long time, it behaves like a resistor with infinite resistance.

Initially, the capacitor has no charge, so the potential difference across it, using the capacitance formula $\Delta V=\frac{Q}{C}$, is zero. On the other side, this capacitor is in parallel with the $5-{\rm \Omega}$ resistor.

Recall that when two electronic components (e.g., a capacitor or resistor) are in parallel, the potential drop across them is the same. According to this rule, the potential difference across the $5-{\rm \Omega}$ resistor is also zero. Applying Ohm's law, $\Delta V=IR$, we find that the current flowing through this resistor must also be zero.

Consequently, the current $I_2$ shown in the circuit, immediately after closing the switch, must be zero. In this situation, the $5-{\rm \Omega}$ resistor is removed and the circuit converts to the following

In this case, as you can see, $I_1$ shows the total current through the battery with $r=0$ whose value is determined by the following formula \[I=\frac{\mathcal{E}}{r+R_{eq}}=\frac{15}{0+10}=1.5\,{\rm A}\] Thus, just after closing the switch $S$, we have $I_1=1.5\,{\rm A}$ and $I_2=0$. The correct answer is b.

Note that in all AP Physics circuit multiple-choice problems, **just after placing an initially uncharged capacitor in a circuit (like immediately after closing a switch in the circuit), it acts as a typical wire with zero resistance, and subsequently, all branches in parallel with it can be removed from the circuit.**

**Problem (14): In the circuit below, the capacitor is initially uncharged. A long time after closing the switch $S$, find the currents $I_1$ and $I_2$.
a. 1, 1 b. 1.5, 0 c. 0, 1.5 d. 1.5, 3**

**Solution**: This is the same previous question, but now we want to analyze the circuit a long time later.

After a long time, when the switch is closed, the charge accumulation on the capacitor reaches its maximum value. At this moment, this charge, which is built on the plates of the capacitor, impedes completely the charge flowing by the battery (precisely, the current through this branch).

So, the current flowing through this branch is stopped and all total current delivered by the battery (i.e., $I_1$) reaching the junction $A$, flows into the branch where the $5-{\rm \Omega}$ resistor is presented. In other words, $I_1=I_2$.

Thus, we can remove that branch including the capacitor, and find the total current through the circuit. In this case, the two $5-{\rm \Omega}$ and $10-{\rm \Omega}$ resistors are in series with an equivalent resistance of $R_{eq}=5+10=15\,{\rm \Omega}$.

On the other side, the current flowing through the circuit is found as \[I_t=\frac{\mathcal{E}}{r+R_{eq}}=\frac{15}{0+15}=1\,{\rm A}\] Therefore, \[I_1=I_2=I_t=1\,{\rm A}\] The correct answer is a.

In all AP Physics circuit multiple-choice questions, note that, after a long time of placing an initially uncharged capacitor in a circuit, it acts as an open circuit, and we can remove that branch from the circuit.

**Author**: Dr. Ali Nemati

**Page Published**: 10/13/2021

© 2015 All rights reserved. by Physexams.com