Capacitance is a measure of how well a conductor can store electric charge. It is defined as the ratio of the charge \(Q\) on the conductor to the potential difference \(V\) between its surfaces:
\$C=\frac{Q}{V}\$
The SI unit is the farad (F). Think of a capacitor like a water tank: the charge is the water stored, and the voltage is the water pressure. The larger the tank, the more water it can hold at a given pressure – just as a larger capacitance can store more charge at a given voltage.
For an isolated sphere of radius \(R\) in free space, the capacitance depends only on its size:
\$C{\text{sphere}} = 4\pi \varepsilon0 R\$
where \(\varepsilon_0 = 8.85\times10^{-12}\,\text{F/m}\) is the vacuum permittivity.
Example: A sphere with radius \(0.1\,\text{m}\) has
\$C = 4\pi (8.85\times10^{-12}) (0.1) \approx 1.11\times10^{-11}\,\text{F} \;(11.1\,\text{pF}).\$
Two flat plates of area \(A\) separated by a distance \(d\) in a medium of permittivity \(\varepsilon\) form a capacitor with capacitance:
\$C_{\text{parallel}} = \varepsilon \frac{A}{d}\$
If the space between the plates is air, \(\varepsilon \approx \varepsilon_0\).
Example: Two plates \(10\,\text{cm}\times10\,\text{cm}\) (\(A=0.01\,\text{m}^2\)) separated by \(1\,\text{mm}\) (\(d=0.001\,\text{m}\)) give
\$C = (8.85\times10^{-12}) \frac{0.01}{0.001} \approx 8.85\times10^{-11}\,\text{F} \;(88.5\,\text{pF}).\$
| Configuration | Formula | Key Variables |
|---|---|---|
| Isolated Sphere | \(C = 4\pi \varepsilon_0 R\) | \(R\) – radius |
| Parallel Plate | \(C = \varepsilon \dfrac{A}{d}\) | \(A\) – area, \(d\) – separation, \(\varepsilon\) – permittivity |