recall and use W = 21QV = 21CV2

Capacitors and Capacitance – Cambridge International AS & A Level Physics 9702

Learning Objective

Recall and use the expressions for the energy stored in a capacitor and related concepts:

\[

W=\frac12QV=\frac12CV^{2}

\]

1. Fundamental Concepts

  • Capacitance – ability of a device to store charge per unit potential difference.
  • Definition \(C=\dfrac{Q}{V}\) (where \(Q\) is the charge on one plate and \(V\) the potential difference).
  • Parallel‑plate capacitor \(C=\displaystyle\frac{\varepsilon{0}A}{d}\) (\(A\) = plate area, \(d\) = separation, \(\varepsilon{0}=8.85\times10^{-12}\,\text{F m}^{-1}\)).
  • Dielectric material – inserting a dielectric of relative permittivity \(\kappa\) multiplies the capacitance by \(\kappa\):

    \[

    C{\text{new}}=\kappa\,C{\text{vacuum}} .

    \]

  • Series and parallel combinations

    ConfigurationResulting capacitance
    Parallel: \(C{\text{eq}} = C{1}+C_{2}+ \dots\)Capacitances add directly.
    Series: \(\displaystyle\frac{1}{C{\text{eq}}}= \frac{1}{C{1}}+\frac{1}{C_{2}}+\dots\)Reciprocals add.

  • Capacitor in a potential‑divider – two capacitors in series share the total voltage in proportion to the inverse of their capacitances:

    \[

    V{1}=V{\text{total}}\frac{C{2}}{C{1}+C_{2}},\qquad

    V{2}=V{\text{total}}\frac{C{1}}{C{1}+C_{2}} .

    \]

    This is the analogue of a resistive voltage divider (Syllabus 10.3).

  • AC reactance – for a sinusoidal source of angular frequency \(\omega\),

    \[

    X_{C}= \frac{1}{\omega C}\qquad(\text{units }\Omega) .

    \]

    \(X_{C}\) appears in Paper 4 questions on alternating currents.

2. Energy Stored in a Capacitor

Derivation

  1. When a small charge \(dq\) is moved onto a plate that already carries charge \(q\), the instantaneous voltage is \(V=\dfrac{q}{C}\).
  2. The incremental work is

    \[

    dW = V\,dq = \frac{q}{C}\,dq .

    \]

  3. Integrating from an uncharged state (\(q=0\)) to the final charge \(Q\):

    \[

    W = \int_{0}^{Q}\frac{q}{C}\,dq

    = \frac{1}{2}\frac{Q^{2}}{C}

    = \frac12 QV

    = \frac12 CV^{2}.

    \]

    The factor \(\tfrac12\) arises because the voltage rises linearly from 0 to its final value.

Energy density

For a uniform electric field between the plates,

\[

u = \frac{W}{\text{volume}} = \frac12\varepsilon_{0}E^{2},

\qquad\text{with }E=\frac{V}{d}.

\]

This form is useful when comparing capacitors with other energy‑storage media.

3. Discharging a Capacitor – RC Time Constant

  • RC circuit – a resistor \(R\) in series with a capacitor \(C\).
  • Time constant \(\tau = RC\) (the time for the voltage to fall to \(e^{-1}\) of its initial value).
  • Discharge equations

    \[

    V(t)=V_{0}\,e^{-t/RC},\qquad

    Q(t)=Q_{0}\,e^{-t/RC}.

    \]

Example – Discharge

A 47 µF capacitor charged to 12 V is connected across a 10 kΩ resistor. Find the voltage after 0.5 s.

  1. \(\tau = RC = (10\,000\;\Omega)(47\times10^{-6}\,\text{F}) = 0.47\;\text{s}\).
  2. \(V(0.5) = 12\,e^{-0.5/0.47} \approx 12\,e^{-1.06} \approx 4.2\;\text{V}.\)

4. Units and Typical Ranges (A‑Level)

QuantitySymbolSI unitTypical range
CapacitanceCfarad (F)pF – µF (parallel‑plate), mF – F (electrolytic)
ChargeQcoulomb (C)10⁻⁹ – 10⁻³ C
VoltageVvolt (V)1 – 500 V
EnergyWjoule (J)10⁻⁹ – 10⁻¹ J
ResistanceRohm (Ω)10 Ω – 10 MΩ (typical for RC circuits)
Angular frequency\(\omega\)rad s\(^{-1}\)10 – 10⁴ (AC circuits)

5. Worked Examples

5.1 Energy Stored

Problem: A 47 µF capacitor is charged to 12 V. Calculate the energy stored.

  1. Use \(W = \dfrac12 CV^{2}\).
  2. \[

    W = \frac12 (47\times10^{-6}\,\text{F})(12\;\text{V})^{2}

    = \frac12 (47\times10^{-6})(144)

    \approx 3.4\times10^{-3}\,\text{J}.

    \]

  3. The capacitor stores about 3.4 mJ of energy.

5.2 Series–Parallel Combination

Problem: Two capacitors, \(C{1}=2.0\;\mu\text{F}\) and \(C{2}=3.0\;\mu\text{F}\), are connected in series, then this combination is placed in parallel with a third capacitor \(C_{3}=5.0\;\mu\text{F}\). Find the equivalent capacitance.

  1. Series part: \(\displaystyle\frac{1}{C{s}}=\frac{1}{C{1}}+\frac{1}{C_{2}}

    =\frac{1}{2.0}+\frac{1}{3.0}=0.833\;\mu\text{F}^{-1}\)

     \(\Rightarrow C_{s}=1.20\;\mu\text{F}\).

  2. Parallel addition: \(C{\text{eq}} = C{s}+C_{3}=1.20+5.0=6.20\;\mu\text{F}\).

5.3 AC Reactance

Problem: A 10 µF capacitor is connected to a 50 Hz AC supply. Find its reactance.

  1. \(\omega = 2\pi f = 2\pi(50)=314\;\text{rad s}^{-1}\).
  2. \(X_{C}= \dfrac{1}{\omega C}= \dfrac{1}{314\times10^{-5}} \approx 318\;\Omega.\)

6. Common Mistakes & How to Avoid Them

  • Leaving out the factor \(\tfrac12\) – it originates from the integration of a linearly increasing voltage.
  • Using the source voltage instead of the actual voltage across the capacitor when it is only partially charged.
  • Failing to convert units (µF → F, kΩ → Ω, µH → H) before substitution.
  • Mixing up symbols: \(C\) for capacitance, \(R\) for resistance, \(X_{C}\) for reactance.
  • Treating series and parallel formulas for resistors as if they were the same for capacitors; remember the reciprocal rule for series.

7. Practical Investigation (AO3 Skill)

Objective: Measure the capacitance of an unknown parallel‑plate capacitor using the RC‑discharge method.

  1. Charge the unknown capacitor to a known voltage \(V_{0}\) (e.g., 10 V) with a DC supply.
  2. Connect a known resistor \(R\) (e.g., 10 kΩ) in series and start a timer the instant the circuit is closed.
  3. Record the voltage across the capacitor at regular intervals (e.g., every 0.1 s) using a digital voltmeter.
  4. Plot \(\ln\!\bigl(V/V_{0}\bigr)\) against time. The plot should be a straight line with slope \(-1/RC\).
  5. Calculate the capacitance:

    \[

    C = -\frac{1}{R\,\text{slope}} .

    \]

  6. Compare the result with a direct reading from a capacitance meter and discuss sources of error (instrument resolution, lead resistance, leakage, stray capacitance).

8. Links to Other Syllabus Areas

  • Energy stored in a capacitor → 19.2 (energy concepts).
  • RC time constant → 20.5 (electromagnetic induction) and 21 (alternating currents).
  • Energy density → 22 (energy of photons & comparison of storage media).
  • Capacitor potential divider → 10.3 (potential dividers).
  • AC reactance → 21.2 (reactive components in AC circuits).

9. Quick Revision Checklist

  1. Write the definition \(C = Q/V\) and the parallel‑plate formula \(C=\varepsilon_{0}A/d\).
  2. State the effect of a dielectric: \(C_{\text{new}}=\kappa C\).
  3. Recall series and parallel combination rules for capacitors.
  4. Remember the three equivalent energy expressions and the \(\tfrac12\) factor.
  5. State the energy‑density formula \(u=\tfrac12\varepsilon_{0}E^{2}\).
  6. Give the RC time constant \(\tau = RC\) and the discharge equation \(V(t)=V_{0}e^{-t/RC}\).
  7. Write the AC reactance \(X_{C}=1/(\omega C)\).
  8. Check units: \(C\) in farads, \(W\) in joules, \(\tau\) in seconds, \(X_{C}\) in ohms.
  9. Complete a numerical problem for (a) energy storage, (b) RC discharge, and (c) AC reactance.
  10. Outline the practical method for measuring an unknown capacitance and list at least three possible error sources.