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Tab Electronics Guide to Understanding Electricity ... - Sciences Club

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Transis<strong>to</strong>rs<br />

179<br />

will be very stable as illustrated, because the voltage gain associated with<br />

the DC quiescent operational levels is held at 10, but it will not be very<br />

repeatable.<br />

Repeatability applies <strong>to</strong> the capability of being able <strong>to</strong> reproduce the<br />

identical set of operating characteristics within multiple identical circuits.<br />

For example, suppose you constructed the circuit of Fig. 6-7f, compared<br />

the input signal <strong>to</strong> the output signal, and discovered the actual AC<br />

voltage gain <strong>to</strong> be 180. If you then removed Q1 from the circuit and<br />

replaced it with another identical 2N3904 transis<strong>to</strong>r, would the AC voltage<br />

gain still be 180 In all probability, it would not. Transis<strong>to</strong>rs are not<br />

manufactured with exact beta values; rather, they are specified as meeting<br />

a required range or minimum beta value. Two identical transis<strong>to</strong>rs<br />

with the same part number could vary by more than 100% in their actual<br />

beta values. Since the AC voltage gain of Fig. 6-7f is largely dependent on<br />

the beta value of Q1, you could construct a dozen identical circuit copies<br />

of Fig. 6-7f and achieve variable AC voltage gains ranging from 120 <strong>to</strong> 250.<br />

Therefore, the repeatability of such a circuit is said <strong>to</strong> be poor.<br />

In its simplest form, you can think of any single-stage transis<strong>to</strong>r<br />

amplifier circuit as a “block” with an input and an output. Like all electronic<br />

circuits having inputs or outputs, there will always be some finite<br />

input impedance and output impedance. So far in this section, you have<br />

examined the internal functions of transis<strong>to</strong>r amplifiers, but it is also<br />

important <strong>to</strong> understand the effect such amplifiers have on external<br />

devices or circuits.<br />

Referring back <strong>to</strong> Fig. 6-7e, the AC signal source in this illustration<br />

could represent a wide variety of devices. It could be a lab signal genera<strong>to</strong>r,<br />

a previous transis<strong>to</strong>r amplifier stage, a signal output from a radio,<br />

the electrical “pickup” from an electric guitar, and the list goes on and<br />

on. It represents any conceivable AC voltage that you want <strong>to</strong> amplify<br />

for any conceivable reason. Regardless of what this AC signal source represents,<br />

it will have an output impedance. In order for transis<strong>to</strong>r amplifiers<br />

<strong>to</strong> function well in a practical manner, the output impedance of<br />

the intended signal source must be compatible with the input impedance<br />

of the transis<strong>to</strong>r amplifier. Otherwise, your intended amplifier may<br />

turn out <strong>to</strong> be an attenua<strong>to</strong>r (i.e., a signal reducer).<br />

Before going in<strong>to</strong> a detailed description of input and output impedances,<br />

it is important <strong>to</strong> understand that all power supplies look like a<br />

low impedance path <strong>to</strong> circuit common (or ground potential) <strong>to</strong> AC signals.<br />

In other words, the internal impedance of all high-quality power<br />

supplies must be very low. As a means of understanding this principle,<br />

you can try a little experiment with a common 9-volt transis<strong>to</strong>r battery

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