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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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Active Element (<strong>Op</strong> Amp) Impact on <strong>the</strong> Oscillator<br />

<strong>the</strong> feedback loop, to automatic ga<strong>in</strong> control (AGC) loops, to limit<strong>in</strong>g by external components<br />

such as resistors and diodes. Consideration must also be given to <strong>the</strong> change <strong>in</strong><br />

ga<strong>in</strong> due to temperature variations and component tolerances, and <strong>the</strong> level of circuit<br />

complexity will be determ<strong>in</strong>ed based on <strong>the</strong> required stability of <strong>the</strong> ga<strong>in</strong>. <strong>The</strong> more stable<br />

<strong>the</strong> ga<strong>in</strong>, <strong>the</strong> better <strong>the</strong> purity of <strong>the</strong> s<strong>in</strong>e wave output.<br />

15.5 Active Element (<strong>Op</strong> Amp) Impact on <strong>the</strong> Oscillator<br />

Up to now, it has been assumed that <strong>the</strong> op amp has an <strong>in</strong>f<strong>in</strong>ite bandwidth and <strong>the</strong> output<br />

is not frequency dependent. In reality, <strong>the</strong> op amp has many poles, but it has been compensated<br />

so that <strong>the</strong>y are dom<strong>in</strong>ated by a s<strong>in</strong>gle pole over <strong>the</strong> specified bandwidth. Thus<br />

Aβ, is now frequency dependant through <strong>the</strong> op amp ga<strong>in</strong> term, A. Equation 15–2 shows<br />

this dependance, where a is <strong>the</strong> maximum open loop ga<strong>in</strong>, ω a is <strong>the</strong> dom<strong>in</strong>ant pole frequency,<br />

and ω is <strong>the</strong> frequency of <strong>the</strong> signal. Figure 15–3 graphically depicts <strong>the</strong> frequency<br />

dependence of <strong>the</strong> op amp ga<strong>in</strong> and phase. <strong>The</strong> closed loop ga<strong>in</strong>, A CL = 1/β does not<br />

conta<strong>in</strong> any poles or zeros and its <strong>the</strong>refore constant over frequency to <strong>the</strong> po<strong>in</strong>t where<br />

it impacts <strong>the</strong> op amp open-loop ga<strong>in</strong> at ω 3dB. Here, <strong>the</strong> signal amplitude is attenuated<br />

by 3 dB and <strong>the</strong> phase shift <strong>in</strong>troduced by <strong>the</strong> op amp is 45°. <strong>The</strong> amplitude and phase<br />

really beg<strong>in</strong> to change one decade below this po<strong>in</strong>t at 0.1 ω 3dB, and <strong>the</strong> phase will cont<strong>in</strong>ue<br />

to shift until it has reached 90° at <strong>10</strong> ω 3dB, one decade beyond <strong>the</strong> 3–dB po<strong>in</strong>t. <strong>The</strong> ga<strong>in</strong><br />

cont<strong>in</strong>ues to roll off at –20 dB/decade until o<strong>the</strong>r poles and zeros come <strong>in</strong>to play. <strong>The</strong> higher<br />

<strong>the</strong> closed-loop g<strong>in</strong>, <strong>the</strong> earlier A CL <strong>in</strong>tercepts <strong>the</strong> op amp ga<strong>in</strong>.<br />

A CL <br />

A<br />

1 A <br />

1<br />

<br />

1 1<br />

<br />

A<br />

ACLideal 1 ACLideal AOL S<strong>in</strong>e Wave Oscillators<br />

(15–2)<br />

<strong>The</strong> phase shift contributed by <strong>the</strong> op amp will impact <strong>the</strong> performance of <strong>the</strong> oscillator<br />

circuit by lower<strong>in</strong>g <strong>the</strong> oscillation frequency, and <strong>the</strong> reduction <strong>in</strong> A CL can make Aβ < 1 and<br />

<strong>the</strong> oscillator will not oscillate.<br />

15-5

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