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Introduction to SAT II Physics - FreeExamPapers

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capacitance is halved. The proportionality constant between C and A/d is<br />

, called the<br />

permittivity of free space, which we encountered in the previous chapter in relation <strong>to</strong><br />

Coulomb’s constant. In case you forgot, C 2 /N · m 2 .<br />

The unit of capacitance is the farad (F). One farad is equal <strong>to</strong> one coulomb per volt. Most<br />

capaci<strong>to</strong>rs have very small capacitances, which are usually given in microfarads, where 1<br />

µF = 10 –6 F.<br />

Energy<br />

To move a small amount of negative charge from the positive plate <strong>to</strong> the negative plate of<br />

a capaci<strong>to</strong>r, an external agent must do work. This work is the origin of the energy s<strong>to</strong>red<br />

by the capaci<strong>to</strong>r.<br />

If the plates have a charge of magnitude q, the potential difference is . If q = 0,<br />

and work is done <strong>to</strong> add charge until q = Q, the <strong>to</strong>tal work required is:<br />

This is the energy s<strong>to</strong>red by the capaci<strong>to</strong>r. Manipulating this equation and the equation<br />

for capacitance,<br />

, we can derive a number of equivalent forms:<br />

Equivalent Capacitance<br />

Like resis<strong>to</strong>rs, capaci<strong>to</strong>rs can be arranged in series or in parallel. The rule for adding<br />

capacitance is the reverse of adding resistance:<br />

Capaci<strong>to</strong>rs in series add like resis<strong>to</strong>rs in parallel, and capaci<strong>to</strong>rs in parallel add like<br />

resis<strong>to</strong>rs in series.<br />

For two capaci<strong>to</strong>rs in series:<br />

For two capaci<strong>to</strong>rs in parallel:<br />

EXAMPLE<br />

237

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