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

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250 Chapter Eight<br />

of Q4 and Q6 will be at about 18 volts also (minus a small drop across<br />

their associated emitter resis<strong>to</strong>rs). If a positive-going AC signal is applied<br />

<strong>to</strong> the input of this amplifier, transis<strong>to</strong>rs Q4 and Q6 will current-amplify<br />

this signal. However, as soon as the AC signal goes in<strong>to</strong> the negative<br />

region, the signal applied <strong>to</strong> the base of Q4 will drop below 18 volts,<br />

causing Q4 and Q6 <strong>to</strong> go in<strong>to</strong> cu<strong>to</strong>ff. Therefore, Q4 and Q6 are only<br />

amplifying about half of the audio signal (i.e., the positive half-cycles of<br />

the audio AC signal). Since transis<strong>to</strong>rs Q5 and Q7 are PNP devices, with<br />

their associated collec<strong>to</strong>rs tied <strong>to</strong> circuit common, they are currentamplifying<br />

the negative half-cycles of the audio AC signal, in a directly<br />

inverse fashion as Q4 and Q6. Simply stated, all audio signal voltages<br />

above 18 volts are amplified by Q4 and Q6, while all audio signal voltages<br />

below 18 volts are amplified by Q5 and Q7. Consequently, the<br />

entire amplified audio signal is summed at the positive plate of C4.<br />

Note that resis<strong>to</strong>r R7 is connected from the amplifier’s output back <strong>to</strong><br />

the “inverting” side of the input differential amplifier (i.e., the base of<br />

Q2). R7 is a negative-feedback resis<strong>to</strong>r. As you recall, the audio signal voltage<br />

at the collec<strong>to</strong>r of Q3 is in phase with the audio input signal. Q4,<br />

Q5, Q6, and Q7 are all connected as common-collec<strong>to</strong>r amplifiers (i.e.,<br />

the input is applied <strong>to</strong> the bases with the output taken from the emitters).<br />

Since common-collec<strong>to</strong>r amplifiers are noninverting, the audio signal<br />

at the amplifier’s output remains in phase with the input signal.<br />

Therefore, the noninverted output signal that R7 applies back <strong>to</strong> the<br />

inverting input of the differential amplifier is negative feedback. Negative<br />

feedback in this circuit establishes the voltage gain, increases linearity<br />

(i.e., decreases dis<strong>to</strong>rtion), and helps stabilize the quiescent voltage<br />

levels. The voltage gain (A e<br />

) of this amplifier is approximately equal <strong>to</strong> R7<br />

divided by the parallel resistance of R5 and R6 (i.e., about 10).<br />

Capaci<strong>to</strong>r C4, like C1, is a coupling capaci<strong>to</strong>r, serving <strong>to</strong> block the quiescent<br />

18-volt DC level from being applied <strong>to</strong> the speaker. Note, however,<br />

that the value of C4 is very large compared <strong>to</strong> the value of C1. This is<br />

necessary because the impedance of most speakers is only about 8 ohms.<br />

Therefore, in order <strong>to</strong> provide a time constant long enough <strong>to</strong> pass lowfrequency<br />

audio signals, the capacity of C4 must be much greater.<br />

Finally, resis<strong>to</strong>r R13 and capaci<strong>to</strong>r C3 form an output circuit that is<br />

commonly referred <strong>to</strong> as a Zobel network. The purpose of a Zobel network<br />

is <strong>to</strong> “counteract” the effect of typical speaker coil inductances,<br />

which could have a destabilizing effect on the amplifier circuitry.<br />

As you may have noted, the Fig. 8-8 amplifier consists of three basic<br />

stages, commonly referred <strong>to</strong> as the input stage (Q1 and Q2), the voltage<br />

amplifier stage (Q3), and the output stage (Q4, Q4, Q6, and Q7). Virtually

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