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www.play-hookey.com | Fri, 09-03-2010 |
| Digital | Logic Families | Digital Experiments | Analog | Analog Experiments | DC Theory | AC Theory | Optics | Computers | Semiconductors | Test HTML | ||
| Direct Links to Other Oscillators Pages: | |
|---|---|
| Introduction to Oscillators: | [What is an Oscillator?] [How Oscillators are Classified] |
| Audio Oscillators: | [Phase Shift Oscillator] [Quadrature Oscillator] [Wien Bridge Oscillator] [Function Generator] |
| LC-based RF Oscillators: | [The Hartley Oscillator] [The Colpitts Oscillator] [The Clapp Oscillator] [The Armstrong Oscillator] |
| Crystal Oscillators: | [The Crystal as a Circuit Element] [Crystal-Controlled Logic Oscillator] [The Pierce Oscillator] |
| More to come soon... | |
| The Clapp Oscillator |
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The circuit shown to the right is a variation of the Colpitts
oscillator first introduced in 1948 by James K. Clapp. A number of
circuits of this type were introduced by different authors at around the
same time, but Mr. Clapp's name stuck, and this circuit is now commonly
known as the Clapp oscillator.
The Clapp oscillator is distinguished from the Colpitts oscillator by the addition of C0 in series with L. This additional capacitor has several effects on the oscillator circuit. The signal voltage divider formed by C1 and C2 is unchanged, and these capacitors are fixed in value. Therefore the amount of energy fed back to sustain oscillations is the same at any frequency, so the amplitude of the signal is not affected much by a change in frequency. In addition, stray capacitances in the transistor have less effect on the operating frequency, which now depends on the series combination of all three capacitors.
The circuit still oscillates at a frequency of
ω = 2πf = 1/
,
but now C0 is part of C in that expression. If C0 is
made variable, it can control the frequency of oscillation without
changing the feedback ratio or the stability of the overall circuit.
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