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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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6.1 Introduction<br />

Development of <strong>the</strong> Non Ideal <strong>Op</strong> Amp<br />

Equations<br />

Ron Manc<strong>in</strong>i<br />

<strong>Chapter</strong> 6<br />

<strong>The</strong>re are two types of error sources <strong>in</strong> op amps, and <strong>the</strong>y fall under <strong>the</strong> general classification<br />

of dc and ac errors. Examples of dc errors are <strong>in</strong>put offset voltage and <strong>in</strong>put bias current.<br />

<strong>The</strong> dc errors stay constant over <strong>the</strong> usable op amp frequency range; <strong>the</strong>refore, <strong>the</strong><br />

<strong>in</strong>put bias current is <strong>10</strong> pA at 1 kHz and it is <strong>10</strong> pA at <strong>10</strong> kHz. Because of <strong>the</strong>ir constant<br />

and controlled behavior, dc errors are not considered until later chapters.<br />

AC errors are flighty, so we address <strong>the</strong>m here by develop<strong>in</strong>g a set of nonideal equations<br />

that account for ac errors. <strong>The</strong> ac errors may show up under dc conditions, but <strong>the</strong>y get<br />

worse as <strong>the</strong> operat<strong>in</strong>g frequency <strong>in</strong>creases. A good example of an ac error is common–<br />

mode rejection ration (CMRR). Most op amps have a guaranteed CMRR specification,<br />

but this specification is only valid at dc or very low frequencies. Fur<strong>the</strong>r <strong>in</strong>spection of <strong>the</strong><br />

data sheet reveals that CMRR decreases as operat<strong>in</strong>g frequency <strong>in</strong>creases. Several o<strong>the</strong>r<br />

specifications that fall <strong>in</strong>to <strong>the</strong> category of ac specifications are output impedance,<br />

power-supply rejection-ratio, peak-to-peak output voltage, differential ga<strong>in</strong>, differential<br />

phase, and phase marg<strong>in</strong>.<br />

Differential ga<strong>in</strong> is <strong>the</strong> most important ac specification because <strong>the</strong> o<strong>the</strong>r ac specifications<br />

are derived from <strong>the</strong> differential ga<strong>in</strong>. Until now, differential ga<strong>in</strong> has been called op amp<br />

ga<strong>in</strong> or op amp open loop ga<strong>in</strong>, and we shall cont<strong>in</strong>ue with that term<strong>in</strong>ology. Let <strong>the</strong> data<br />

sheet call it differential ga<strong>in</strong>.<br />

As shown <strong>in</strong> prior chapters, when frequency <strong>in</strong>creases, <strong>the</strong> op amp ga<strong>in</strong> decreases and<br />

errors <strong>in</strong>crease. This chapter develops <strong>the</strong> equations that illustrate <strong>the</strong> effects of <strong>the</strong> ga<strong>in</strong><br />

changes. We start with a review of <strong>the</strong> basic canonical feedback system stability because<br />

<strong>the</strong> op amp equations are developed us<strong>in</strong>g <strong>the</strong> same techniques.<br />

Amplifiers are built with active components such as transistors. Pert<strong>in</strong>ent transistor parameters<br />

like transistor ga<strong>in</strong> are subject to drift and <strong>in</strong>itial <strong>in</strong>accuracies from many<br />

sources, so amplifiers be<strong>in</strong>g built from <strong>the</strong>se components are subject to drift and <strong>in</strong>accura-<br />

6-1

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