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Starting electronics<br />

Figure 4.3<br />

(Left) an axial capacitor and (right) a radial capacitor<br />

Measuring up<br />

Capacitance values are measured in a unit called the farad<br />

(named after the scientist: Faraday) and given the symbol:<br />

F. We’ll define exactly what the farad is later, suffice to say<br />

here that it is a very large unit. Typical capacitors have values<br />

much, much smaller. Fractions such as a millionth of a<br />

farad (that is, one microfarad: 1 µF), a thousand millionth<br />

of a farad (that is, one nanofarad: 1 nF), or one million millionth<br />

of a farad (that is, one picofarad: 1 pF) are common.<br />

Sometimes, like the Ω or R of resistances, the unit F is omitted<br />

— 15 n, instead of 15 nF, say.<br />

The circuit for our first experiment is shown in Figure 4.4. You<br />

should see that it bears a striking resemblance to the voltage<br />

divider resistor circuits we looked at last chapter, except that<br />

a capacitor has taken the place of one of the resistors. Also<br />

included in the circuit of Figure 4.4 is a switch. In the last<br />

chapter’s circuits, no switch was used as we were only interested<br />

in static conditions after the circuits were connected.<br />

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