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Physics (AS & A Level) 9702 · Chapter 19

Capacitance

Capacitance of isolated spheres and parallel plates, capacitors in series and parallel, energy stored from the area under a graph, and exponential discharge through a resistor with the time constant RC.

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19.1 Capacitors and capacitance

Capacitance is the charge stored per unit potential:

C=QVC = \frac{Q}{V}

The unit is the farad, where 1 F = 1 C/V.

  • For a parallel plate capacitor, it is the charge on one plate per unit p.d. between the plates.
  • For an isolated spherical conductor, it is the charge on it per unit potential at its surface. Combining C=Q/VC = Q/V with V=Q/(4πε0r)V = Q/(4\pi\varepsilon_0 r) gives C=4πε0rC = 4\pi\varepsilon_0 r.

A capacitor's plates hold equal and opposite charges. The net charge is zero, and QQ means the charge on one plate.

Capacitors in series and parallel

In parallel, the p.d. is the same across each, and the charges add: Q=Q1+Q2Q = Q_1 + Q_2. Dividing by VV gives:

C=C1+C2+…C = C_1 + C_2 + \dots

In series, each capacitor holds the same charge, and the p.d.s add: V=V1+V2V = V_1 + V_2. Dividing by QQ gives:

1C=1C1+1C2+…\frac{1}{C} = \frac{1}{C_1} + \frac{1}{C_2} + \dots

19.2 Energy stored in a capacitor

Charging a capacitor means moving charge against an increasing p.d., so the work done is the area under the potential–charge graph, which is a triangle.

A straight-line graph of potential difference against charge through the origin, with the triangular area under it marked as the energy stored

A straight-line graph of potential difference against charge through the origin, with the triangular area under it marked as the energy stored

W=12QV=12CV2=Q22CW = \tfrac{1}{2}QV = \tfrac{1}{2}CV^2 = \frac{Q^2}{2C}

It is not QVQV, because the p.d. builds up from zero. The cell does transfer QVQV, and half of that goes to heat in the circuit's resistance, whatever the size of the resistance.

19.3 Discharging a capacitor

When a capacitor discharges through a resistor, the current is large at first, because the p.d. is large. As the charge falls, the p.d. falls and the current falls. So the rate of loss of charge is proportional to the charge left, which gives an exponential decay.

x=x0e−t/RCx = x_0 e^{-t/RC}

where xx can be the charge, the p.d. or the current.

An exponential decay curve of charge against time, with the time constant RC marked where the charge has fallen to 37 percent

An exponential decay curve of charge against time, with the time constant RC marked where the charge has fallen to 37 percent

The time constant

The time constant is:

τ=RC\tau = RC

It is the time for the charge to fall to 1/e1/e, or about 37%, of its starting value. After 5RC5RC the capacitor is effectively discharged. A larger RR makes the current smaller, and a larger CC means there is more charge to remove, so both make discharge slower.

Finding the time constant from a graph

  • From an exponential curve, read the time at which the value falls to 37%.
  • Taking natural logs gives ln⁡x=ln⁡x0−t/RC\ln x = \ln x_0 - t/RC. So a graph of ln⁡V\ln V against tt is a straight line with gradient −1/RC-1/RC.
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