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Op Amps for Everyone - The Repeater Builder's Technical ...

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Bandwidth<br />

A <br />

aR G<br />

R F R G<br />

(9–2)<br />

Equation 9–2 is rewritten below as Equations 9–3 and 9–4 <strong>for</strong> the noninverting and inverting<br />

circuits respectively. In each case, the symbol G CLNI and G CLI represent the closed<br />

loop gain <strong>for</strong> the noninverting and inverting circuits respectively.<br />

A <br />

a<br />

R F R G<br />

a<br />

R G<br />

G CLNI (9–3)<br />

(9–4)<br />

A <br />

a<br />

R F R G<br />

a<br />

G CLI<br />

1<br />

R G<br />

In both cases the loop gain decreases as the closed loop gain increases, thus all VFA errors<br />

increase as the closed loop gain increases. <strong>The</strong> error increase is mathematically<br />

coupled to the closed loop gain equation, so there is no working around this fact. For the<br />

VFA, effective bandwidth decreases as the closed loop gain increases because the loop<br />

gain decreases as the closed loop gain increases.<br />

A plot of the VFA loop gain, closed loop gain, and error is given in Figure 9–3. Referring<br />

to Figure 9–3, the direct gain, A, is the op amp open loop gain, a, <strong>for</strong> a noninverting op<br />

amp. <strong>The</strong> direct gain <strong>for</strong> an inverting op amp is (a(Z F /(Z G + Z F ))). <strong>The</strong> Miller effect causes<br />

the direct gain to fall off at high frequencies, thus error increases as frequency increases<br />

because the effective loop gain decreases. At a given frequency, the error also increases<br />

when the closed loop gain is increased.<br />

20 LOG A<br />

Gain in dB<br />

20 LOG (1 + Aβ)<br />

Direct Gain<br />

20 LOG(G CL )<br />

CLOSED LOOP GAIN<br />

LOG f<br />

Figure 9–3. VFA Gain versus Frequency<br />

9-4

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