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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 OUT V TH<br />

R4 V RTH R3 R4 R2 R4 R1 R2 R1R2 R<br />

R 3 R4 1R2 Review of Circuit <strong>The</strong>ory<br />

<strong>The</strong>ven<strong>in</strong>’s <strong>The</strong>orem<br />

(2–15)<br />

<strong>The</strong> circuit analysis is done <strong>the</strong> hard way <strong>in</strong> Figure 2–<strong>10</strong>, so you can see <strong>the</strong> advantage<br />

of us<strong>in</strong>g <strong>The</strong>ven<strong>in</strong>’s <strong>The</strong>orem. Two loop currents, I 1 and I 2, are assigned to <strong>the</strong> circuit.<br />

<strong>The</strong>n <strong>the</strong> loop Equations 2–16 and 2–17 are written.<br />

Figure 2–<strong>10</strong>. Analysis Done <strong>the</strong> Hard Way<br />

V<br />

R1<br />

I1<br />

R2<br />

V I 1 R 1 R 2 I 2 R 2<br />

R3<br />

I 2 R 2 R 3 R 4 I 1 R 2<br />

I2<br />

R4<br />

VOUT<br />

(2–16)<br />

(2–17)<br />

Equation 2–17 is rewritten as Equation 2–18 and substituted <strong>in</strong>to Equation 2–16 to obta<strong>in</strong><br />

Equation 2–19.<br />

I 1 I 2<br />

R 2 R 3 R 4<br />

R 2<br />

V I2 R2 R3 R4R R 1 R 2 I2R2 2<br />

(2–18)<br />

(2–19)<br />

<strong>The</strong> terms are rearranged <strong>in</strong> Equation 2–20. Ohm’s law is used to write Equation 2–21,<br />

and <strong>the</strong> f<strong>in</strong>al substitutions are made <strong>in</strong> Equation 2–22.<br />

I 2 <br />

V<br />

R2R3R 4 R<br />

R 1 R 2 R2 2<br />

V OUT I 2 R 4<br />

V OUT V<br />

R 4<br />

R2R3R R 4 1R 2<br />

R2 R 2<br />

(2–20)<br />

(2–21)<br />

(2–22)<br />

This is a lot of extra work for no ga<strong>in</strong>. Also, <strong>the</strong> answer is not <strong>in</strong> a usable form because<br />

<strong>the</strong> voltage dividers are not recognizable, thus more algebra is required to get <strong>the</strong> answer<br />

<strong>in</strong>to usable form.<br />

2-7

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