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Starting electronics<br />

Note that current (and voltage) scales read in the opposite<br />

direction to the resistance scale we used in the last chapter,<br />

and they are linear. This makes them considerably easier to<br />

use than resistance scales and they are also more accurate as<br />

you can more easily judge a value if the pointer falls between<br />

actual marks on the scale.<br />

Voltages<br />

When you measure voltages with your multi-meter the same<br />

procedure should be followed, using the highest voltage<br />

ranges first and stepping down as required. The voltages<br />

you are measuring here are all direct voltages as they are<br />

taken from a 9 V d.c. battery. So you needn’t bother using the<br />

three highest d.c. voltage ranges on the multi-meter, as your<br />

9 V battery can’t generate a high enough voltage to damage<br />

the meter anyway. Also, don’t bother using the a.c. voltage<br />

ranges as they’re — pretty obviously — for measuring only<br />

alternating (that is, a.c.) voltages.<br />

As an example you can build the circuit of Figure 3.9 up on<br />

your breadboard, shown in Figure 3.11. What is the measured<br />

voltage? It should be about 4.5 V.<br />

Now measure the voltage across the other resistor — it’s<br />

also about 4.5 V. Well, that figures, doesn’t it? There’s about<br />

4.5 V across each resistor, so there is a total of 2 x 4.5 V that<br />

is, 9 V across them both: the voltage of the battery. This has<br />

demonstrated that resistors in series act as a voltage divider<br />

or a potential divider, dividing up the total voltage applied<br />

68

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