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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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RG<br />

55.2 kΩ<br />

2.5 V<br />

RF<br />

1.5 MΩ<br />

+5 V<br />

_<br />

+<br />

TLV2471<br />

Figure 15–14. Phase Shift Oscillator (S<strong>in</strong>gle <strong>Op</strong> Amp)<br />

R R R<br />

<strong>10</strong> kΩ <strong>10</strong> kΩ <strong>10</strong> kΩ<br />

C<br />

Time = 500 µs/div<br />

Figure 15–15. Output of <strong>the</strong> Circuit <strong>in</strong> Figure 15–14<br />

VOUT = 1 V/div<br />

A A 1<br />

RCs 13 <strong>10</strong> nF C <strong>10</strong> nF C <strong>10</strong> nF<br />

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

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

VOUT<br />

(15–<strong>10</strong>)<br />

<strong>The</strong> normal assumption is that <strong>the</strong> phase shift sections are <strong>in</strong>dependent of each o<strong>the</strong>r.<br />

<strong>The</strong>n Equation 15–<strong>10</strong> is written. <strong>The</strong> loop phase shift is –180 when <strong>the</strong> phase shift of<br />

each section is –60, and this occurs when ω = 2πf = 1.732/RC because <strong>the</strong> tangent of<br />

60 = 1.732. <strong>The</strong> magnitude of β at this po<strong>in</strong>t is (1/2) 3, so <strong>the</strong> ga<strong>in</strong>, A, must be equal to<br />

8 for <strong>the</strong> system ga<strong>in</strong> to be equal to one.<br />

<strong>The</strong> oscillation frequency with <strong>the</strong> component values shown <strong>in</strong> Figure 15–14 is 3.76 kHz<br />

ra<strong>the</strong>r than <strong>the</strong> calculated oscillation frequency of 2.76 kHz as shown <strong>in</strong> Figure 15–14.<br />

Also, <strong>the</strong> ga<strong>in</strong> required to start oscillation is 27 ra<strong>the</strong>r than <strong>the</strong> calculated ga<strong>in</strong> of 8. <strong>The</strong>se<br />

15-15

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