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Cadence OrCAD PCB Designer

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2. The base–emitter junction of a transistor is a forward-biassed diode (hence the arrow on<br />

its symbol) and therefore has a voltage of V be<br />

≈ 0.7V across it. Calculate the voltage on<br />

the emitter.<br />

Hint for demonstrators.<br />

2.0 V ❦<br />

3. We now know the voltage across the resistor R 4<br />

. Calculate the current through it.<br />

Hint for demonstrators.<br />

11.1 mA (the aim was 10 mA) ❦<br />

4. The current into the base of a transistor is much smaller than the other two currents, so<br />

the current flowing into the collector is nearly equal to that flowing out of the emitter.<br />

Calculate the voltage dropped across R 3<br />

and hence the voltage on the collector.<br />

Hint for demonstrators.<br />

4.3 V across R 3<br />

so V c = 5.7V (the aim was 6 V) ❦<br />

This has shown why the four resistors are needed but not the capacitors. What is the expression<br />

for the impedance of a capacitor (remember that it is complex), and how does its magnitude<br />

depend on frequency? The function of the capacitors in this circuit is to allow high frequencies<br />

to pass – the signals that we wish to amplify – but to block the steady voltages that set the bias<br />

point.<br />

• We have seen that the base of the transistor is kept at a particular voltage by the potential<br />

divider, which sets the bias point. The capacitor C 1<br />

on the input isolates this voltage from<br />

the previous stage of the system but lets the signal through.<br />

• Look at the circuit through which the input signal flows. It passes ‘through’ the capacitor<br />

C 1<br />

, through the base–emitter junction of the transistor, through R 4<br />

and C 2<br />

in parallel, and<br />

back to the ground connection of the input. This shows that R 4<br />

is in series with the input<br />

and will reduce its magnitude. We really want all the voltage to be applied across the<br />

base–emitter junction, where it will be amplified by the transistor. However, we can’t<br />

simply get rid of R 4<br />

because it is needed to set the bias point – it determines the current<br />

through the transistor, as you saw above. The solution is to put the bypass capacitor C 2<br />

across the resistor.<br />

The bias has zero frequency so it all flows through the resistor. The signal has a ‘high’ frequency<br />

so most of it flows through the capacitor, which should have a much smaller impedance than<br />

the resistor. Ideally the impedance of C 2<br />

should obey |Z C<br />

( f )| ≪ R 4<br />

for all frequencies in the<br />

signal. Is this true for the values in figure 1?<br />

Hint for demonstrators. No! At the lowest frequency of 10 Hz, X C<br />

= 1/2π fC = 160kΩ,<br />

which is much larger than R 4<br />

= 180Ω. The capacitor should be a thousand times larger. This<br />

will be shown by the simulation. ❦<br />

Finally, we would like to estimate the voltage gain of the circuit. This needs some background<br />

on transistors that you have not yet covered so I’ll just quote the result. The gain is<br />

given by<br />

V out<br />

= −g m R<br />

V 3<br />

(1)<br />

in<br />

5

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