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Questions on the time constant and exponential decay
The time constant of a resistor-capacitor circuit is the product RC, in seconds, and after one time constant of discharge 37% of the charge is left on the plates. Discharge follows Q = Q₀e^(−t/RC), halving every 0.69RC. Taking natural logs straightens the curve, which is how RC is measured.
19 original questions · 55 marks · the time constant and exponential decay notes · Capacitance
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State the equation for the time constant of a capacitor-resistor circuit and explain what the time constant represents for a discharging capacitor.
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τ = RC (1); the time for the charge (or pd, or current) to fall to 1/e (about 37%) of its initial value (1).A 100 μF capacitor discharges through a 10 kΩ resistor. Calculate the time constant of the circuit.
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τ = RC = 10000 × 100 × 10−6 (1)
τ = 1.0 s (1)Write down the equation for the charge remaining on a capacitor at time t as it discharges through a resistor.
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Q = Q0e−t/RC, where Q0 is the initial charge (1).A capacitor charges through a resistor. State the percentage of its final charge that it has gained one time constant after charging begins.
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63% (the fraction 1 − 1/e) (1).A 47 μF capacitor discharges through a 2.2 MΩ resistor. Calculate the time constant of the circuit.
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τ = RC = 2.2 × 106 × 47 × 10−6 (1)
τ = 103 s (1)A 470 μF capacitor discharges through a 2.2 kΩ resistor. Calculate the time constant and state the fraction of the initial charge that remains after one time constant.
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τ = RC = 2200 × 470 × 10−6 (1)
τ = 1.03 s (1)
After one time constant, Q/Q0 = 1/e ≈ 0.37 (37%) (1).A 100 μF capacitor is charged to 12 V and then discharged through a 47 kΩ resistor. Calculate the potential difference across the capacitor 5.0 s after the discharge begins.
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τ = RC = 47000 × 100 × 10−6 = 4.7 s (1)
V = V0e−t/RC = 12 × e−5.0/4.7 (1)
V = 4.14 V (1)For the circuit in the previous question, calculate the time taken for the potential difference to halve.
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T½ = 0.69RC = 0.69 × 4.7 (1)
T½ = 3.24 s (1)A timing circuit requires a time constant of 2.0 s using a 220 μF capacitor. Calculate the resistance required.
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R = τ/C = 2.0/(220 × 10−6) (1)
R = 9.1 × 103 Ω (9.1 kΩ) (1)In required practical 9 a student discharges a capacitor through a resistor while logging the pd across it. The pd falls from 6.0 V to 2.2 V in 15 s. Show that the time constant of the circuit is about 15 s.
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V = V0e−t/τ, so t/τ = ln(V0/V) (1)
ln(6.0/2.2) = 1.00 (1)
τ = 15/1.00 = 15.0 s ≈ 15 s (1)A capacitor discharges through a 33 kΩ resistor. The pd across it halves every 4.6 s. Determine the capacitance of the capacitor.
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T½ = 0.69RC (1)
C = T½/(0.69R) = 4.6/(0.69 × 33000) (1)
C = 2.0 × 10−4 F (200 μF) (1)A capacitor discharges through a resistor with a time constant of 3.0 s. Determine the time taken for the potential difference across it to fall from 20 V to 5.0 V.
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5.0 = 20e−t/3.0, so e−t/3.0 = 0.25 (1)
t = −3.0 × ln(0.25) (1)
t = 4.16 s (1)A 470 μF capacitor is charged from a 9.0 V supply through a 10 kΩ resistor. Calculate the potential difference across the capacitor 10 s after charging begins.
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τ = RC = 10000 × 470 × 10−6 = 4.7 s (1)
V = V0(1 − e−t/RC) = 9.0 × (1 − e−10/4.7) (1)
V = 7.93 V (1)A student plots ln(V) against time for a discharging capacitor. Explain how the time constant can be determined from this graph.
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Taking logs of V = V0e−t/RC gives ln V = ln V0 − t/RC (1); this is a straight line with gradient −1/RC (1); so the time constant RC is the negative reciprocal of the gradient (1).A student uses required practical 9 to test a capacitor labelled 470 μF with a tolerance of ±20%. The capacitor is discharged through a 10 kΩ resistor, and the graph of ln(V) against t is a straight line of gradient −0.185 s−1. Deduce whether the capacitor is within its stated tolerance.
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The gradient is −1/RC, so RC = 1/0.185 = 5.41 s (1)
C = RC/R = 5.41/10000 = 5.41 × 10−4 F = 541 μF (1)
The tolerance allows 376 μF to 564 μF (1)
541 μF lies inside this range, so the capacitor is within its stated tolerance (1).A capacitor discharges through a resistor. Show that the energy stored falls to about 14% of its initial value after one time constant.
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E = ½Q2/C, so E is proportional to Q2 (1)
After one time constant Q has fallen to Q0/e, so E falls to E0/e2 (1)
1/e2 = 0.135, which is about 14% (1)The manual for a high-voltage supply states that its reservoir capacitor must be left to discharge until less than 1.0% of the initial charge remains before the case is opened. The discharge time constant is 4.0 s. Determine the minimum waiting time.
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Q/Q0 = 0.010 = e−t/τ (1)
t = −4.0 × ln(0.010) = 4.0 × ln(100) (1)
t = 18.4 s (about 4.6 time constants) (1)Describe an experiment to determine the capacitance of an unmarked capacitor by discharging it through a resistor of known resistance. Include the measurements you would take and explain how you would analyse the data to obtain the capacitance.
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Charge the capacitor from a supply, then discharge it through the known resistor with a voltmeter or datalogger connected across the capacitor (or resistor) (1). Record the pd at regular time intervals, using a stopwatch (or the datalogger's clock) started as the discharge begins (1). Plot ln V against t (1); a straight line confirms that the decay is exponential (1). The gradient of the line equals −1/RC (1); so C = −1/(R × gradient), using the known resistance (1).A 100 μF capacitor carrying a charge of 600 μC begins to discharge through a 20 kΩ resistor at t = 0. A student models the discharge step by step from ΔQ/Δt = −Q/CR, using a time step Δt = 0.50 s and holding the rate at its start-of-step value across each step. Calculate the charge left by the model at the end of each of the four steps to t = 2.0 s, compare the final value with the charge given by Q = Q0e−t/CR, and explain the difference.
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CR = 20000 × 100 × 10−6 = 2.0 s, so ΔQ = −(Q/CR)Δt = −Q × 0.50/2.0 = −0.25Q, leaving 0.75Q at the end of each step (1)
Step 1: ΔQ = −150.0 μC, Q = 450.0 μC; step 2: ΔQ = −112.5 μC, Q = 337.5 μC (1)
Step 3: ΔQ = −84.4 μC, Q = 253.1 μC; step 4: ΔQ = −63.3 μC, Q = 189.8 μC (1)
The exponential gives Q = 600 × e−2.0/2.0 = 220.7 μC (1)
The model's 189.8 μC is below the exponential's 220.7 μC, low by about 14% (1)
because the rate is held at its start-of-step value, which is the largest it takes during the step, so every step removes slightly too much charge; a smaller Δt reduces the difference (1)
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