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AP · AP C:E&M · extended response

A discharging capacitor transfers finite energy to a resistor

AP Physics C: Electricity and Magnetism · Original GioPhysics question with a detailed, mark-by-mark answer guide.

Demand
discriminating
Marks
6
Topics
1
Answer
Complete
Explore the question data

Capacitor discharge voltage

Supplied question data. Read the labelled axes and use the observations to test the physical model.

Vertical axis (y): Voltage / V

Capacitor discharge voltageSupplied question data. Read the labelled axes and use the observations to test the physical model. Horizontal axis: Time / s. Vertical axis: Voltage / V. Exact values are available in the data table below.02.557.51001.042.0793.1194.158xy

Horizontal axis (x): Time / s

Reading 1Time / s: 0Voltage / V: 10
Read the exact data as a table
Capacitor discharge voltage — supplied values
Time / sVoltage / V
010
1.3865
2.7722.5
4.1581.25

These are the supplied values, not a worked answer. No fitted trend is drawn.

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extended response6 marks

A 100 μF capacitor initially at 10.0 V discharges through a 20.0 kΩ resistor. The supplied voltages follow V(t) = V0 exp(−t/RC). There is no power supply during discharge. Use ln2 = 0.693 and neglect leakage and meter loading. Supplied data (Time / s; Voltage / V): (0, 10), (1.386, 5), (2.772, 2.5), (4.158, 1.25).

  1. (a)

    Find the time constant, initial current, initial stored energy and time for voltage to reach half its initial value.

    3 marks
  2. (b)

    Find energy remaining and energy dissipated when voltage halves. Derive the energy decay law and explain why current also halves at that time.

    3 marks
Ready to self-mark?Reveal the detailed answer guide
Answer overview(a) RC = 2.0 s; Iinitial = 0.50 mA; Uinitial = 5.0 mJ; voltage half-time = 1.386 s. (b) Remaining energy = 1.25 mJ; dissipated = 3.75 mJ; U = U0 exp(−2t/RC).
01

(a)

3 marks

Find the time constant, initial current, initial stored energy and time for voltage to reach half its initial value.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    The time constant is RC = (2.0×10⁴)(1.0×10⁻⁴) = 2.0 s; initial current magnitude is V0/R = 10/20000 = 0.50 mA.

  2. 2

    Initial energy is ½CV0² = ½(1.0×10⁻⁴)(100) = 0.0050 J.

  3. 3

    Setting V/V0 = 1/2 gives t = RC ln2 = 1.386 s, consistent with the supplied data. The time constant is not the voltage half-time.

02

(b)

3 marks

Find energy remaining and energy dissipated when voltage halves. Derive the energy decay law and explain why current also halves at that time.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    Since U = ½CV² and C is fixed, halving voltage quarters stored energy, leaving 5.0/4 = 1.25 mJ.

  2. 2

    The resistor receives the missing 3.75 mJ as thermal energy. Substitution of V(t) gives U(t) = U0 exp(−2t/RC), so energy decays with a time constant RC/2.

  3. 3

    Ohm's law gives I(t) = V(t)/R, so current halves when voltage halves. Integrating I²R over the full discharge returns the finite initial capacitor energy.

Complete marking guidance

Use these worked steps alongside the part-by-part answers. They explain the method and mark allocation; they do not add extra marks.

  1. The time constant is RC = (2.0×10⁴)(1.0×10⁻⁴) = 2.0 s; initial current magnitude is V0/R = 10/20000 = 0.50 mA.
  2. Initial energy is ½CV0² = ½(1.0×10⁻⁴)(100) = 0.0050 J.
  3. Setting V/V0 = 1/2 gives t = RC ln2 = 1.386 s, consistent with the supplied data. The time constant is not the voltage half-time.
  4. Since U = ½CV² and C is fixed, halving voltage quarters stored energy, leaving 5.0/4 = 1.25 mJ.
  5. The resistor receives the missing 3.75 mJ as thermal energy. Substitution of V(t) gives U(t) = U0 exp(−2t/RC), so energy decays with a time constant RC/2.
  6. Ohm's law gives I(t) = V(t)/R, so current halves when voltage halves. Integrating I²R over the full discharge returns the finite initial capacitor energy.

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