EG1216 · Physics 2 — Electricity & Magnetism
Theme 2 · Electric potential & capacitance

Capacitance & calculating it

Two conductors that store equal and opposite charge make a capacitor. Capacitance is how much charge it holds per volt.

Source: Serway & Jewett, Physics for Scientists and Engineers, 7th ed., §26.1–26.2.

Before you start

What you need first

  • Topic 9 — voltage \(V\), and \(V = Ed\) between parallel plates.
  • Topic 7 — the uniform field of a charged sheet/plate.
  • Powers of ten — µF, nF, pF.

What you'll be able to do

  • Say what a capacitor is and what it stores.
  • Use \(C = Q/V\) (and \(Q = CV\)), and the farad.
  • Use the parallel-plate formula \(C = \varepsilon_0 A/d\).
  • Say what makes a capacitance bigger.

The idea

What is a capacitor?

A capacitor is two conductors (often two plates) with a gap between them. Connect a battery and one plate gains \(+Q\), the other \(-Q\) — the capacitor stores that charge and the energy with it.

Think of it as a tiny tank for charge: a bigger tank holds more charge at the same voltage.
+++ plate area A gap d
Two plates of area \(A\), a gap \(d\) apart, holding \(+Q\) and \(-Q\).

Capacitance — the definition

Capacitance \(C\) measures how much charge a capacitor holds per volt across it:

$$ C = \frac{Q}{V} \qquad\Longleftrightarrow\qquad Q = CV $$
where:
SymbolMeaningSI unit
Ccapacitance (charge stored per volt)F = C/V
Qcharge on each plate (one \(+Q\), one \(-Q\))C
Vvoltage across the platesV
The farad is huge. Real capacitors are far smaller, so you'll see µF \((10^{-6})\), nF \((10^{-9})\), and pF \((10^{-12})\). Convert to farads before using any formula.
📐 Worked example 1

Capacitance and charge stored

(a) A capacitor stores \(Q = 30\ \mu\text{C}\) at \(V = 10\) V — find \(C\). (b) A \(C = 5\ \mu\text{F}\) capacitor is connected to \(V = 12\) V — find the charge stored.

1Capacitance from \(C = Q/V\):
$$ C = \frac{30\times10^{-6}}{10} = 3\times10^{-6}\ \text{F} = 3\ \mu\text{F} $$
2Charge from \(Q = CV\):
$$ Q = (5\times10^{-6})(12) = 6\times10^{-5}\ \text{C} = 60\ \mu\text{C} $$

Capacitance of parallel plates

For two flat plates, the capacitance is set entirely by the geometry — area and gap (with air or vacuum between):

$$ C = \frac{\varepsilon_0 A}{d} $$
where:
SymbolMeaningSI unit
Aarea of each plate
dgap between the platesm
ε₀permittivity of free space \(=8.85\times10^{-12}\)C²/(N·m²)
Bigger plates (large \(A\)) → more room for charge → bigger \(C\). Smaller gap (small \(d\)) → bigger \(C\). Real capacitors use large plates very close together, often rolled into a tiny cylinder.
📐 Worked example 2

A parallel-plate capacitor

Two plates of area \(A = 0.020\) m² sit a gap \(d = 0.0010\) m (1 mm) apart, with air between. Find the capacitance.

1Use \(C = \varepsilon_0 A/d\):
$$ C = \frac{(8.85\times10^{-12})(0.020)}{0.0010} $$
2Work it out:
$$ C \approx 1.8\times10^{-10}\ \text{F} = 180\ \text{pF} $$

✏️ Try it yourself

A parallel-plate capacitor has plates of area \(A = 0.050\) m² with an air gap \(d = 0.0020\) m.

(a) Find its capacitance.
(b) If you halve the gap, what happens to the capacitance?

(a) \(C = \dfrac{\varepsilon_0 A}{d} = \dfrac{(8.85\times10^{-12})(0.050)}{0.0020} \approx 2.2\times10^{-10}\ \text{F} = 220\ \text{pF}.\) (b) \(C\) is inversely proportional to \(d\), so halving the gap doubles \(C\) to about \(440\) pF.

Common mistakes

MistakeFix
Thinking \(C\) depends on \(Q\) or \(V\).\(C\) is fixed by the geometry (\(A\), \(d\)); \(C=Q/V\) just measures it. More \(V\) → proportionally more \(Q\), same \(C\).
Leaving capacitance in µF/pF in a formula.Convert to farads first.
Putting \(d\) on top of the plate formula.\(C = \varepsilon_0 A/d\): the gap is on the bottom — smaller gap, bigger \(C\).
Forgetting both plates carry the same size charge.One plate \(+Q\), the other \(-Q\); "the charge" \(Q\) is that size.

Recap — the whole topic on one screen

IdeaWhat you own now
CapacitorTwo conductors storing \(+Q\) and \(-Q\); a charge "tank."
Capacitance\(C = Q/V\), \(Q = CV\); unit farad (C/V), usually µF–pF.
Parallel plates\(C = \dfrac{\varepsilon_0 A}{d}\) — set by geometry.
Bigger CLarge area, small gap.

Next topic

Capacitors in series & parallel

Wire several capacitors together and they behave like one. Next we find the rules — and meet the circuit symbol for a capacitor.

→ Topic 13 · Capacitors in series & parallel