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

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Superposition<br />

2.6 Superposition<br />

2-8<br />

Superposition is a <strong>the</strong>orem that can be applied to any l<strong>in</strong>ear circuit. Essentially, when<br />

<strong>the</strong>re are <strong>in</strong>dependent sources, <strong>the</strong> voltages and currents result<strong>in</strong>g from each source can<br />

be calculated separately, and <strong>the</strong> results are added algebraically. This simplifies <strong>the</strong> calculations<br />

because it elim<strong>in</strong>ates <strong>the</strong> need to write a series of loop or node equations. An<br />

example is shown <strong>in</strong> Figure 2–11.<br />

V1<br />

Figure 2–11.Superposition Example<br />

R1<br />

R3<br />

V2<br />

R2<br />

VOUT<br />

When V 1 is grounded, V 2 forms a voltage divider with R 3 and <strong>the</strong> parallel comb<strong>in</strong>ation of<br />

R 2 and R 1. <strong>The</strong> output voltage for this circuit (V OUT2) is calculated with <strong>the</strong> aid of <strong>the</strong> voltage<br />

divider equation (2–23). <strong>The</strong> circuit is shown <strong>in</strong> Figure 2–12. <strong>The</strong> voltage divider rule<br />

yields <strong>the</strong> answer quickly.<br />

Figure 2–12. When V 1 is Grounded<br />

V OUT2 V 2<br />

R3<br />

V2 R1 R2 VOUT2<br />

R 1 R 2<br />

R 3 R 1 R 2<br />

(2–23)<br />

Likewise, when V 2 is grounded (Figure 2–13), V 1 forms a voltage divider with R 1 and <strong>the</strong><br />

parallel comb<strong>in</strong>ation of R 3 and R 2, and <strong>the</strong> voltage divider <strong>the</strong>orem is applied aga<strong>in</strong> to calculate<br />

V OUT (Equation 2–24).<br />

Figure 2–13. When V 2 is Grounded<br />

R1<br />

V1 R3 R2 VOUT1

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