Resistor–Capacitor (RC) Circuits

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AP Physics C: Electricity and Magnetism › Resistor–Capacitor (RC) Circuits

Questions 1 - 5
1

Consider the RC circuit shown. A $6.0,\text{V}$ capacitor initially at $6.0,\text{V}$ discharges through $R=3.0,\text{k}\Omega$, $C=100,\mu\text{F}$; what is $V_C$ after $0.60,\text{s}$?

$2.7,\text{V}$

$0.81,\text{V}$

$1.2,\text{V}$

$4.8,\text{V}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically analyzing capacitor discharge in RC circuits. During discharge, voltage follows V(t) = V₀e^(-t/RC), where V₀ is the initial voltage across the capacitor. With R = 3.0 kΩ and C = 100 μF, the time constant is τ = RC = (3.0×10³)(100×10⁻⁶) = 0.30 s, and the capacitor starts at V₀ = 6.0 V. Choice A is correct because after t = 0.60 s (two time constants), V_C = 6.0×e^(-0.60/0.30) = 6.0×e^(-2) = 6.0×0.135 = 0.81 V. Choice B might result from using only one time constant (6.0×e^(-1) ≈ 2.2 V) or calculation error, while choice D might incorrectly use the charging formula. To help students: remember that after two time constants, voltage drops to about 13.5% of initial value (e^(-2) ≈ 0.135), and practice recognizing multiples of the time constant. Watch for confusion between charging and discharging scenarios and ensure proper exponential calculations.

2

Consider the RC circuit shown. A $10,\text{V}$ source charges an initially uncharged $R=5.0,\text{k}\Omega$, $C=100,\mu\text{F}$ capacitor; determine time to reach $6.0,\text{V}$.

$0.46,\text{s}$

$0.51,\text{s}$

$0.25,\text{s}$

$0.92,\text{s}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically determining the time required for a capacitor to reach a specific voltage during charging. For a charging capacitor, V(t) = V₀(1-e^(-t/RC)), which can be rearranged to solve for time: t = -RC×ln(1-V/V₀). With R = 5.0 kΩ, C = 100 μF, the time constant is τ = RC = (5.0×10³)(100×10⁻⁶) = 0.50 s, and we need the time to reach 6.0 V from 0 V with V₀ = 10 V. Choice A is correct because t = -0.50×ln(1-6.0/10) = -0.50×ln(0.40) = -0.50×(-0.916) = 0.46 s. Choice B might result from incorrectly using t = τ×(V/V₀) = 0.50×(6/10) = 0.30 s, assuming linear rather than exponential growth. To help students: practice rearranging exponential equations, use natural logarithms correctly, and understand that reaching 60% of final voltage takes less than one time constant. Watch for algebraic errors when solving exponential equations and confusion about when to use ln versus other operations.

3

Consider the RC circuit shown. A $12,\text{V}$ capacitor initially at $12,\text{V}$ discharges through $R=10,\text{k}\Omega$, $C=10,\mu\text{F}$; what is $V_C$ after $0.050,\text{s}$?

$11,\text{V}$

$4.7,\text{V}$

$7.3,\text{V}$

$9.4,\text{V}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically calculating voltage during capacitor discharge. For a discharging capacitor, V(t) = V₀e^(-t/RC), where V₀ is the initial voltage. With R = 10 kΩ and C = 10 μF, the time constant is τ = RC = (10×10³)(10×10⁻⁶) = 0.10 s, and the capacitor starts at V₀ = 12 V. Choice A is correct because after t = 0.050 s (half a time constant), V_C = 12×e^(-0.050/0.10) = 12×e^(-0.5) = 12×0.606 = 7.3 V. Choice B might result from using the wrong exponential value or calculation error, while choice C might incorrectly apply the charging formula. To help students: memorize that after half a time constant of discharge, voltage drops to about 60.6% of initial value, and practice quick mental calculations with common exponential values. Watch for confusion between charging and discharging formulas and ensure accurate exponential calculations.

4

Consider the RC circuit shown. A precharged capacitor $C=2.0\times10^{-4},\text{F}$ at $9.0,\text{V}$ discharges through $R=1.5,\text{k}\Omega$; what is $V_C$ after $0.30,\text{s}$?

$5.5,\text{V}$

$3.3,\text{V}$

$7.8,\text{V}$

$1.2,\text{V}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically analyzing RC circuits during capacitor discharge. For a discharging capacitor, the voltage follows V(t) = V₀e^(-t/RC), where V₀ is the initial voltage and τ = RC is the time constant. In this circuit with R = 1.5 kΩ and C = 2.0×10⁻⁴ F, the time constant is τ = (1.5×10³)(2.0×10⁻⁴) = 0.30 s, with initial voltage V₀ = 9.0 V. Choice A is correct because after t = 0.30 s (one time constant), V_C = 9.0×e^(-0.30/0.30) = 9.0×e^(-1) = 9.0×0.368 = 3.3 V. Choice B might result from incorrectly using the charging formula (9.0×(1-e^(-1)) ≈ 5.7 V) instead of the discharging formula. To help students: emphasize the difference between charging and discharging equations, and remember that after one time constant of discharge, voltage drops to about 36.8% of initial value. Watch for sign errors and confusion about which formula applies to which scenario.

5

Consider the RC circuit shown: a capacitor initially at 10 V discharges through $R=4.7\times10^{3},\Omega$ with $C=4.7\times10^{-6},\text{F}$. What is the remaining voltage across the capacitor after discharging for 0.022 s?

$V_C\approx 9.5,\text{V}$

$V_C\approx 0.47,\text{V}$

$V_C\approx 3.7,\text{V}$

$V_C\approx 6.3,\text{V}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically analyzing RC circuits during capacitor discharge. For a discharging capacitor, the voltage decreases exponentially according to V(t) = V₀e^(-t/RC), where V₀ is the initial voltage. In this circuit, with R = 4.7×10³ Ω and C = 4.7×10⁻⁶ F, the time constant is τ = RC = 0.0221 s, and we need the voltage after t = 0.022 s. Choice A is correct because V(0.022) = 10×e^(-0.022/0.0221) = 10×e^(-0.995) = 10×0.370 ≈ 3.7 V. Choice B is incorrect because it appears to use the charging formula V = V₀(1-e^(-t/RC)) instead of the discharging formula, giving approximately 6.3 V. To help students: clearly distinguish between charging and discharging formulas, emphasize that discharge starts from initial voltage and decays to zero, and practice identifying initial conditions. Watch for: mixing up charging and discharging equations, which is the most common error in RC circuit problems.