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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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S<strong>in</strong>e Wave Oscillator Circuits<br />

15-14<br />

C1<br />

0.1 µF<br />

+<br />

−<br />

R2<br />

11.3 kΩ<br />

VC1<br />

−<br />

RS<br />

<strong>10</strong> kΩ<br />

+<br />

J1<br />

VREF = 2.5 V<br />

R1 <strong>10</strong> kΩ<br />

RG2 <strong>10</strong> kΩ<br />

RG1<br />

<strong>10</strong> kΩ<br />

Figure 15–12. <strong>Wien</strong> Bridge Oscillator with AGC<br />

VD1<br />

+ −<br />

D1 1N4933<br />

C<br />

Time = 500 µs/div<br />

Figure 15–13. Output of <strong>the</strong> Circuit <strong>in</strong> Figure 15–12<br />

15.7.2 Phase Shift Oscillator, S<strong>in</strong>gle Amplifier<br />

VOUT = 1 V/div<br />

R<br />

RF 18.2 kΩ<br />

_<br />

+<br />

R<br />

C<br />

VOUT<br />

Phase shift oscillators have less distortion than <strong>the</strong> <strong>Wien</strong> bridge oscillator, coupled with<br />

good frequency stability. A phase shift oscillator can be built with one op amp as shown<br />

<strong>in</strong> figure 15–14. Three RC sections are cascaded to get <strong>the</strong> steep dφ/dω slope as described<br />

<strong>in</strong> Section 15–3 to get a stable oscillation frequency. Any less and <strong>the</strong> oscillation<br />

frequency is high and <strong>in</strong>terferes with <strong>the</strong> op amp BW limitations.

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