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Starting electronics<br />

voltage (about 3 V). Figure 5.3(a) shows an equivalent circuit<br />

to that of Figure 5.2 for the times during which the electronic<br />

switch of the 555 is off.<br />

You should be able to work out that the capacitor C1 of the<br />

circuit is connected through resistors R1 and R2 to the positive<br />

power supply rail. The time constant τ 1<br />

of this part of the<br />

circuit is therefore given by:<br />

When the voltage across the switch rises to about 6 V, however,<br />

the switch turns on (as shown in Figure 5.3(b), forming<br />

a short circuit across the capacitor and resistor, R2. The<br />

capacitor now discharges with a time constant given by:<br />

Of course, when the discharging voltage across the switch<br />

falls to about 3 V, the switch turns off again, and the capacitor<br />

charges up once more. The process repeats indefinitely,<br />

with the switch turning on and off at a rate determined by the<br />

two time constants. Because of this up and down effect such<br />

oscillators are often known as relaxation oscillators.<br />

As you might expect the circuit integrated within the 555 is<br />

not just that simple and there are many other parts to it (one<br />

part, for example, converts the charging and discharging exponential<br />

voltages into only two definite voltages — 9 V and 0 V<br />

— so that the 555’s output signal is a square wave, as shown<br />

in Figure 5.3(c). But the basic idea of the astable multi-vibrator<br />

formed by a 555 is just as we’ve described here.<br />

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