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Physics · Ch 2 — Electrostatic Potential and Capacitance

Capacitors and Capacitance

2.12

Capacitors and Capacitance

A capacitor is a device purpose-built to store electric charge (and, along with it, electrical energy), consisting of nothing more than two conductors -- called its plates or electrodes -- placed close to one another and kept electrically insulated from each other, either by vacuum, by air, or by a dielectric medium filling the gap between them. When connected to a source of potential difference (such as a battery), one plate accumulates a charge +Q+Q and the other an equal and opposite charge −Q-Q, with a corresponding potential difference VV established between them.

Definition of capacitance. For a GIVEN capacitor, experiment (and theory) shows that the charge QQ it holds is always directly proportional to the potential difference VV applied across it -- doubling VV exactly doubles QQ, and so on. The constant of proportionality is called the capacitor's capacitance:

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

Capacitance is a property of the capacitor's own GEOMETRY (the size and shape of its plates, and the separation between them) and of the MEDIUM filling the gap between the plates -- it does not depend on the particular charge QQ or voltage VV used at any given moment, exactly as a container's volume does not depend on how much liquid happens to be poured into it at a given time. Different geometries and media give different capacitance values, but for one fixed capacitor, CC stays the same constant regardless of how it is charged.

SI unit. The unit of capacitance is the farad (F\text{F}), defined so that 1 F=1 C/V1\ \text{F} = 1\ \text{C/V}: a capacitance of one farad means one coulomb of charge produces a potential difference of just one volt across the capacitor. A farad is, in practice, an enormous unit -- a capacitor storing a genuinely useful, everyday amount of charge for even a modest voltage typically has a capacitance measured in microfarads (1 μF=10−6 F1\ \mu\text{F} = 10^{-6}\ \text{F}), nanofarads (1 nF=10−9 F1\ \text{nF} = 10^{-9}\ \text{F}), or picofarads (1 pF=10−12 F1\ \text{pF} = 10^{-12}\ \text{F}), which is why these smaller submultiples, rather than the farad itself, are the units actually printed on most real capacitors. …