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

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Block Diagram Math and Manipulations<br />

5-4<br />

R<br />

Figure 5–5. Multiloop Feedback System<br />

+<br />

Block diagram reduction rules:<br />

–<br />

+<br />

R<br />

+<br />

+<br />

G1<br />

–<br />

H1<br />

G4<br />

Comb<strong>in</strong>e cascade blocks.<br />

Comb<strong>in</strong>e parallel blocks.<br />

Elim<strong>in</strong>ate <strong>in</strong>terior feedback loops.<br />

Shift summ<strong>in</strong>g po<strong>in</strong>ts to <strong>the</strong> left.<br />

Shift takeoff po<strong>in</strong>ts to <strong>the</strong> right.<br />

Repeat until canonical form is obta<strong>in</strong>ed.<br />

H2<br />

G1G4(G2 + G3)<br />

1 – G1G4H1<br />

Figure 5–6 gives <strong>the</strong> block diagram transforms. <strong>The</strong> idea is to reduce <strong>the</strong> diagram to its<br />

canonical form because <strong>the</strong> canonical feedback loop is <strong>the</strong> simplest form of a feedback<br />

loop, and its analysis is well documented. All feedback systems can be reduced to <strong>the</strong><br />

canonical form, so all feedback systems can be analyzed with <strong>the</strong> same math. A canonical<br />

loop exists for each <strong>in</strong>put to a feedback system; although <strong>the</strong> stability dynamics are <strong>in</strong>dependent<br />

of <strong>the</strong> <strong>in</strong>put, <strong>the</strong> output results are <strong>in</strong>put dependent. <strong>The</strong> response of each <strong>in</strong>put<br />

of a multiple <strong>in</strong>put feedback system can be analyzed separately and added through superposition.<br />

H2<br />

G3<br />

G2<br />

C<br />

+<br />

+<br />

C

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