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"Chapter 1 - The Op Amp's Place in the World" - HTL Wien 10

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Figure 15–17. Output of <strong>the</strong> Circuit Figure 15–16<br />

15.7.4 Bubba Oscillator<br />

VOUT = 200 mV/div<br />

Time = 500 µs/div<br />

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

<strong>The</strong> bubba oscillator <strong>in</strong> Figure 15–18 is ano<strong>the</strong>r phase shift oscillator, but it takes advantage<br />

of <strong>the</strong> quad op amp package to yield some unique advantages. Four RC sections<br />

require 45 phase shift per section, so this oscillator has an excellent dφ/dt result<strong>in</strong>g <strong>in</strong><br />

m<strong>in</strong>imized frequency drift. <strong>The</strong> RC sections each contribute 45 phase shift, so tak<strong>in</strong>g outputs<br />

from alternate sections yields low impedance quadrature outputs. When an output<br />

is taken from each op amp, <strong>the</strong> circuit delivers four 45 phase shifted s<strong>in</strong>e waves. <strong>The</strong> loop<br />

equation is given <strong>in</strong> Equation 15–11. When ω = 1/RCs, Equation 15–11 reduces to Equations<br />

15–12 and 15–13.<br />

A A 1<br />

RCs 14 | | 1<br />

j 4 4<br />

tan 1 (1) 45 °<br />

<br />

<br />

<br />

1<br />

<br />

1<br />

4<br />

4<br />

2<br />

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

(15–11)<br />

(15–12)<br />

(15–13)<br />

15-17

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