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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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Voltage-Feedback <strong>Op</strong> Amp Compensation<br />

Lead Compensation<br />

Ga<strong>in</strong> compensation works for <strong>in</strong>vert<strong>in</strong>g or non<strong>in</strong>vert<strong>in</strong>g op amp circuits because <strong>the</strong> loop<br />

ga<strong>in</strong> equation conta<strong>in</strong>s <strong>the</strong> closed-loop ga<strong>in</strong> parameters <strong>in</strong> both cases. When <strong>the</strong> closedloop<br />

ga<strong>in</strong> is <strong>in</strong>creased, <strong>the</strong> accuracy and <strong>the</strong> bandwidth decrease. As long as <strong>the</strong> application<br />

can stand <strong>the</strong> higher ga<strong>in</strong>, ga<strong>in</strong> compensation is <strong>the</strong> best type of compensation to use.<br />

Uncompensated versions of normally <strong>in</strong>ternally compensated op amps are offered for<br />

sale as stable op amps with m<strong>in</strong>imum ga<strong>in</strong> restrictions. As long as ga<strong>in</strong> <strong>in</strong> <strong>the</strong> circuit you<br />

design exceeds <strong>the</strong> ga<strong>in</strong> specified on <strong>the</strong> data sheet, this is economical and a safe mode<br />

of operation.<br />

7.6 Lead Compensation<br />

Sometimes lead compensation is forced on <strong>the</strong> circuit designer because of <strong>the</strong> parasitic<br />

capacitance associated with packag<strong>in</strong>g and wir<strong>in</strong>g op amps. Figure 7–13 shows <strong>the</strong> circuit<br />

for lead compensation; notice <strong>the</strong> capacitor <strong>in</strong> parallel with R F. That capacitor is often<br />

made by parasitic wir<strong>in</strong>g and <strong>the</strong> ground plane, and high frequency circuit designers go<br />

to great lengths to m<strong>in</strong>imize or elim<strong>in</strong>ate it. What is good <strong>in</strong> one sense is bad <strong>in</strong> ano<strong>the</strong>r,<br />

because add<strong>in</strong>g <strong>the</strong> parallel capacitor is a good way to stabilize <strong>the</strong> op amp and reduce<br />

noise. Let us analyze <strong>the</strong> stability first, and <strong>the</strong>n we will analyze <strong>the</strong> closed-loop performance.<br />

VIN<br />

Figure 7–13. Lead-Compensation Circuit<br />

RG<br />

+<br />

_ a<br />

RF<br />

C<br />

VOUT<br />

<strong>The</strong> loop equation for <strong>the</strong> lead-compensation circuit is given by Equation 7–12.<br />

A RG RG RF RFCs 1<br />

RG RFCs 1<br />

<br />

<br />

<br />

K<br />

s s 1 <br />

2 <br />

(7–12)<br />

<strong>The</strong> compensation capacitor <strong>in</strong>troduces a pole and zero <strong>in</strong>to <strong>the</strong> loop equation. <strong>The</strong> zero<br />

always occurs before <strong>the</strong> pole because R F >R F||R G. When <strong>the</strong> zero is properly placed it<br />

cancels out <strong>the</strong> τ 2 pole along with its associated phase shift. <strong>The</strong> orig<strong>in</strong>al transfer function<br />

is shown <strong>in</strong> Figure 7–14 drawn <strong>in</strong> solid l<strong>in</strong>es. When <strong>the</strong> R FC zero is placed at ω = 1/τ 2, it<br />

cancels out <strong>the</strong> τ 2 pole caus<strong>in</strong>g <strong>the</strong> bode plot to cont<strong>in</strong>ue on a slope of –20 dB/decade.<br />

When <strong>the</strong> frequency gets to ω = 1/(R F||RG)C, this pole changes <strong>the</strong> slope to –40 dB/decade.<br />

Properly placed, <strong>the</strong> capacitor aids stability, but what does it do to <strong>the</strong> closed-loop<br />

<br />

7-13

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