"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
"Chapter 1 - The Op Amp's Place in the World" - HTL Wien 10
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
Stability<br />
9.4 Stability<br />
9-6<br />
Substitut<strong>in</strong>g this value <strong>in</strong>to Equation 9–6 yields Equation 9–7, and Equation 9–7 is almost<br />
identical to Equation 9–6. R B does cause some <strong>in</strong>teraction between <strong>the</strong> loop ga<strong>in</strong> and <strong>the</strong><br />
transimpedance, but because <strong>the</strong> <strong>in</strong>teraction is secondary <strong>the</strong> CFA ga<strong>in</strong> falls off with a<br />
faster slope.<br />
A Z<br />
1.1 R F<br />
(9–7)<br />
<strong>The</strong> direct ga<strong>in</strong> of a VFA starts fall<strong>in</strong>g off early, often at <strong>10</strong> Hz or <strong>10</strong>0 Hz, but <strong>the</strong> transimpedance<br />
of a CFA does not start fall<strong>in</strong>g off until much higher frequencies. <strong>The</strong> VFA is<br />
constra<strong>in</strong>ed by <strong>the</strong> ga<strong>in</strong>-bandwidth limitation imposed by <strong>the</strong> closed loop ga<strong>in</strong> be<strong>in</strong>g <strong>in</strong>corporated<br />
with<strong>in</strong> <strong>the</strong> loop ga<strong>in</strong>. <strong>The</strong> CFA, with <strong>the</strong> exception of <strong>the</strong> effects of R B, does not<br />
have this constra<strong>in</strong>t. This adds up to <strong>the</strong> CFA be<strong>in</strong>g <strong>the</strong> superior high frequency amplifier.<br />
Stability <strong>in</strong> a feedback system is def<strong>in</strong>ed by <strong>the</strong> loop ga<strong>in</strong>, and no o<strong>the</strong>r factor, <strong>in</strong>clud<strong>in</strong>g<br />
<strong>the</strong> <strong>in</strong>puts or type of <strong>in</strong>puts, affects stability. <strong>The</strong> loop ga<strong>in</strong> for a VFA is given <strong>in</strong> Equation<br />
9–2. Exam<strong>in</strong><strong>in</strong>g Equation 9–2 we see that <strong>the</strong> stability of a VFA is depends on two items;<br />
<strong>the</strong> op amp transfer function, a, and <strong>the</strong> ga<strong>in</strong> sett<strong>in</strong>g components, Z F/Z G.<br />
<strong>The</strong> op amp conta<strong>in</strong>s many poles, and if it is not <strong>in</strong>ternally compensated, it requires external<br />
compensation. <strong>The</strong> op amp always has at least one dom<strong>in</strong>ant pole, and <strong>the</strong> most<br />
phase marg<strong>in</strong> that an op amp has is 45°. Phase marg<strong>in</strong>s beyond 60° are a waste of op<br />
amp bandwidth. When poles and zeros are conta<strong>in</strong>ed <strong>in</strong> Z F and Z G, <strong>the</strong>y can compensate<br />
for <strong>the</strong> op amp phase shift or add to its <strong>in</strong>stability. In any case, <strong>the</strong> ga<strong>in</strong> sett<strong>in</strong>g components<br />
always affect stability. When <strong>the</strong> closed-loop ga<strong>in</strong> is high, <strong>the</strong> loop ga<strong>in</strong> is low, and low loop<br />
ga<strong>in</strong> circuits are more stable than high loop ga<strong>in</strong> circuits.<br />
Wir<strong>in</strong>g <strong>the</strong> op amp to a pr<strong>in</strong>ted circuit board always <strong>in</strong>troduces components formed from<br />
stray capacitance and <strong>in</strong>ductance. Stray <strong>in</strong>ductance becomes dom<strong>in</strong>ant at very high frequencies,<br />
hence, <strong>in</strong> VFAs, it does not <strong>in</strong>terfere with stability as much as it does with signal<br />
handl<strong>in</strong>g properties. Stray capacitance causes stability to <strong>in</strong>crease or decrease depend<strong>in</strong>g<br />
on its location. Stray capacitance from <strong>the</strong> <strong>in</strong>put or output lead to ground <strong>in</strong>duces <strong>in</strong>stability,<br />
while <strong>the</strong> same stray capacitance <strong>in</strong> parallel with <strong>the</strong> feedback resistor <strong>in</strong>creases<br />
stability.<br />
<strong>The</strong> loop ga<strong>in</strong> for a CFA with no <strong>in</strong>put buffer output impedance, R B, is given <strong>in</strong> Equation<br />
9–6. Exam<strong>in</strong><strong>in</strong>g Equation 9–6 we see that <strong>the</strong> stability of a CFA depends on two items:<br />
<strong>the</strong> op amp transfer function, Z, and <strong>the</strong> ga<strong>in</strong> sett<strong>in</strong>g component, Z F. <strong>The</strong> op amp conta<strong>in</strong>s<br />
many poles, thus <strong>the</strong>y require external compensation. Fortunately, <strong>the</strong> external compensation<br />
for a CFA is done with Z F. <strong>The</strong> factory applications eng<strong>in</strong>eer does extensive<br />
test<strong>in</strong>g to determ<strong>in</strong>e <strong>the</strong> optimum value of R F for a given ga<strong>in</strong>. This value should be used<br />
<strong>in</strong> all applications at that ga<strong>in</strong>, but <strong>in</strong>creased stability and less peak<strong>in</strong>g can be obta<strong>in</strong>ed<br />
by <strong>in</strong>creas<strong>in</strong>g R F. Essentially this is sacrific<strong>in</strong>g bandwidth for lower frequency performance,<br />
but <strong>in</strong> applications not requir<strong>in</strong>g <strong>the</strong> full bandwidth, it is a wise tradeoff.