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"Chapter 1 - The Op Amp's Place in the World" - HTL Wien 10

"Chapter 1 - The Op Amp's Place in the World" - HTL Wien 10

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V OUT1 V 1<br />

R 2 R 3<br />

R 1 R 2 R 3<br />

Calculation of a Saturated Transistor Circuit<br />

Review of Circuit <strong>The</strong>ory<br />

(2–24)<br />

After <strong>the</strong> calculations for each source are made <strong>the</strong> components are added to obta<strong>in</strong> <strong>the</strong><br />

f<strong>in</strong>al solution (Equation 2–25).<br />

R2 R3 R1 R2 VOUT V1 V2 R1 R2 R3 R3 R1 R2 (2–25)<br />

<strong>The</strong> reader should analyze this circuit with loop or node equations to ga<strong>in</strong> an appreciation<br />

for superposition. Aga<strong>in</strong>, <strong>the</strong> superposition results come out as a simple arrangement that<br />

is easy to understand. One looks at <strong>the</strong> f<strong>in</strong>al equation and it is obvious that if <strong>the</strong> sources<br />

are equal and opposite polarity, and when R 1 = R 3, <strong>the</strong>n <strong>the</strong> output voltage is zero. Conclusions<br />

such as this are hard to make after <strong>the</strong> results of a loop or node analysis unless considerable<br />

effort is made to manipulate <strong>the</strong> f<strong>in</strong>al equation <strong>in</strong>to symmetrical form.<br />

2.7 Calculation of a Saturated Transistor Circuit<br />

<strong>The</strong> circuit specifications are: when V IN = 12 V, V OUT

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