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"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 />

large odd and even harmonics. <strong>The</strong> feedback resistor was <strong>the</strong>n adjusted ±1%. Figure<br />

15–9 shows <strong>the</strong> output voltage waveforms. <strong>The</strong> distortion grew as <strong>the</strong> saturation <strong>in</strong>creased<br />

with <strong>in</strong>creas<strong>in</strong>g R F, and oscillations ceased when R F was decreased by more<br />

than 0.8%.<br />

RG<br />

<strong>10</strong> kΩ<br />

C<br />

RF = 2RG<br />

20 kΩ<br />

+5 V<br />

_ TLV2471<br />

VOUT<br />

+<br />

R<br />

<strong>10</strong> kΩ<br />

<strong>10</strong> nF C<br />

VREF<br />

0.833 V<br />

<strong>10</strong> nF<br />

Figure 15–8. F<strong>in</strong>al <strong>Wien</strong> Bridge Oscillator Circuit<br />

VCC = 5 V<br />

VREF = 0.833 V<br />

RG = <strong>10</strong>.0 kΩ<br />

VOUT = 2 V/div<br />

Figure 15–9. <strong>Wien</strong> Bridge Output Waveforms<br />

+ –<br />

Time = 500 µs/div<br />

R<br />

<strong>10</strong> kΩ<br />

S<strong>in</strong>e Wave Oscillators<br />

V+1%<br />

RF = 20.20 kΩ<br />

VI<br />

RF = 20 kΩ<br />

V–0.8%<br />

RF = 19.84 kΩ<br />

Apply<strong>in</strong>g nonl<strong>in</strong>ear feedback can m<strong>in</strong>imize <strong>the</strong> distortion <strong>in</strong>herent <strong>in</strong> <strong>the</strong> basic <strong>Wien</strong> bridge<br />

circuit. A nonl<strong>in</strong>ear component such as an <strong>in</strong>candescent lamp can be substituted <strong>in</strong>to<br />

15-11

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