AP Physics 2: Algebra-Based Practice Quiz: Resistor-Capacitor (RC) Circuits
Written by AP Content Team, Verified for 2026 AP Exams, Last updated: May 2026
Test your understanding with short quizzes. This quiz has 15 questions to check your progress.
Question 1 of 15
All Questions (15)
A) 0.97 F
B) 1.0 F
C) 6.0 F
D) 10.0 F
Correct Answer: D
For capacitors connected in parallel, the equivalent capacitance is the sum of the individual capacitances. Relevant equation: $C_{eq,p}=\sum_{i}C_i$. Therefore, $C_{eq} = 2 F + 3 F + 5 F = 10.0 F$.
A) 0.5 F
B) 2 F
C) 9 F
D) 18 F
Correct Answer: B
For capacitors connected in series, the inverse of the equivalent capacitance is equal to the sum of the inverses of the individual capacitances. Relevant equation: $\frac{1}{C_{eq,s}}=\sum_{i}\frac{1}{C_i}$. So, $\frac{1}{C_{eq}} = \frac{1}{3 F} + \frac{1}{6 F} = \frac{2}{6 F} + \frac{1}{6 F} = \frac{3}{6 F} = \frac{1}{2 F}$. Therefore, $C_{eq} = 2 F$.
A) The total time required for the capacitor to become fully charged.
B) The maximum charge the capacitor can store.
C) A measure of how quickly the capacitor charges or discharges.
D) The equivalent resistance of the circuit.
Correct Answer: C
The provided content defines the time constant τ of an RC circuit as 'a measure of how quickly the capacitor will charge or discharge'. It is a characteristic time, not the total time to charge.
A) 0.4 s
B) 2.5 s
C) 14 s
D) 40 s
Correct Answer: D
The time constant is calculated using the formula τ = R_eq * C_eq. In this simple series circuit, R_eq = 10 Ω and C_eq = 4 F. Thus, τ = (10 Ω)(4 F) = 40 s.
A) It acts like a short circuit with zero resistance.
B) It acts like an open circuit with zero current in its branch.
C) It continuously draws the maximum possible current.
D) Its capacitance effectively becomes zero.
Correct Answer: B
The content states that after a long time, a charging capacitor approaches a state of being fully charged, at which there is zero current in the circuit branch where the capacitor is located. This behavior is equivalent to an open circuit.
A) 1 s
B) 6 s
C) 25 s
D) 30 s
Correct Answer: C
First, find the equivalent capacitance of the parallel capacitors: C_eq = C1 + C2 = 2 F + 3 F = 5 F. Then, calculate the time constant using τ = R_eq * C_eq. The equivalent resistance is 5 Ω. Therefore, τ = (5 Ω)(5 F) = 25 s.
A) 5 s
B) 72 s
C) 120 s
D) 300 s
Correct Answer: B
First, find the equivalent capacitance for the series capacitors: 1/C_eq = 1/10 F + 1/15 F = 3/30 F + 2/30 F = 5/30 F = 1/6 F. So, C_eq = 6 F. Then, calculate the time constant: τ = R_eq * C_eq = (12 Ω)(6 F) = 72 s.
A) τ/4
B) τ/2
C) τ
D) 2τ
Correct Answer: C
The time constant is given by τ = RC. The new resistance is R' = 2R and the new capacitance is C' = C/2. The new time constant is τ' = R'C' = (2R)(C/2) = RC = τ. The time constant remains unchanged.
A) 0 A
B) 2 A
C) 3 A
D) 6 A
Correct Answer: B
After a very long time, the capacitor is fully charged and acts as an open circuit, meaning no current flows through its branch. The circuit then behaves as if the 2 Ω and 4 Ω resistors are in series. The total equivalent resistance is R_eq = 2 Ω + 4 Ω = 6 Ω. The current from the battery is given by Ohm's Law: I = V/R_eq = 12V / 6Ω = 2 A.
A) 3 F
B) 4 F
C) 6 F
D) 12 F
Correct Answer: A
First, calculate the equivalent capacitance of the parallel combination of C2 and C3: C_p = C2 + C3 = 2 F + 4 F = 6 F. Now, this 6 F equivalent capacitor is in series with C1 (6 F). Calculate the final equivalent capacitance: 1/C_eq = 1/C1 + 1/C_p = 1/6 F + 1/6 F = 2/6 F = 1/3 F. Therefore, C_eq = 3 F.
A) τ_X = τ_Y
B) τ_X = 2τ_Y
C) τ_Y = 2τ_X
D) τ_X = 4τ_Y
Correct Answer: A
The time constant for Circuit X is τ_X = RC. The time constant for Circuit Y is τ_Y = (2R)(C/2) = RC. Therefore, the time constants are equal, τ_X = τ_Y.
A) always greater than the largest individual capacitance.
B) always equal to the sum of the individual capacitances.
C) always less than the smallest individual capacitance.
D) always equal to the average of the individual capacitances.
Correct Answer: C
The formula for series capacitors is $\frac{1}{C_{eq,s}}=\sum_{i}\frac{1}{C_i}$. Summing the reciprocals results in a total reciprocal that is larger than any individual reciprocal. Consequently, the equivalent capacitance itself must be smaller than any of the individual capacitances.
A) 40 s
B) 100 s
C) 250 s
D) 400 s
Correct Answer: C
First, find the equivalent resistance and capacitance. The resistors are in series, so R_eq = R1 + R2 = 4 Ω + 6 Ω = 10 Ω. The capacitors are in parallel, so C_eq = C1 + C2 = 5 F + 20 F = 25 F. The time constant is τ = R_eq * C_eq = (10 Ω)(25 F) = 250 s.
A) 0 V
B) 3.33 V
C) 6.67 V
D) 10 V
Correct Answer: D
After a very long time, the capacitor becomes fully charged, and the current in the series circuit drops to zero. With zero current (I=0), the potential drop across the resistor is V_R = IR = (0 A)(3 Ω) = 0 V. According to Kirchhoff's loop rule, the sum of voltage drops around the loop must equal the battery voltage. Since the voltage drop across the resistor is zero, the entire battery voltage must be across the capacitor. Therefore, V_C = 10 V.
A) It is the sum of the inverses of the individual capacitances.
B) It is the inverse of the sum of the individual capacitances.
C) It is the product of the individual capacitances.
D) It is the sum of the individual capacitances.
Correct Answer: D
The provided content explicitly states that 'The equivalent capacitance of a set of capacitors in parallel is the sum of the individual capacitances.' The relevant equation is $C_{eq,p}=\sum_{i}C_i$.