Salam Academy
Paper 4 · Module

Capacitance

3 subtopics≈ 105 min in total
  1. Capacitors and capacitance

    A capacitor stores separated charge: +Q+Q on one plate, −Q-Q on the other. Its capacitance is the charge stored per unit p.d.: C=QVC=\dfrac QV, measured in farads (F). An isolated sphere also has capacitance, C=4πε0rC=4\pi\varepsilon_0r. Capacitors in parallel add: C=C1+C2C=C_1+C_2. In series, reciprocals add: 1C=1C1+1C2\dfrac1C=\dfrac1{C_1}+\dfrac1{C_2}, the opposite of resistors.

    ≈ 35 min
  2. Energy stored in a capacitor

    As a capacitor charges, each new bit of charge is pushed onto the plates against a rising p.d., so the p.d.–charge graph is a straight line through the origin. The energy stored is the area under it: W=12QV=12CV2=Q22CW=\tfrac12QV=\tfrac12CV^2=\dfrac{Q^2}{2C}. A battery charging a capacitor supplies QVQV, but only half is stored; the other half is dissipated in the circuit resistance.

    ≈ 30 min
  3. Discharging a capacitor

    When a capacitor discharges through a resistor, the current is proportional to the charge remaining, so charge, p.d. and current all decay exponentially: x=x0e−t/RCx=x_0e^{-t/RC}. The time constant τ=RC\tau=RC is the time for any of them to fall to 1e\dfrac1e (37%37\%) of its starting value. A graph of ln⁡V\ln V against tt is a straight line with gradient −1RC-\dfrac1{RC}.

    ≈ 40 min