Butler oscillator

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Single transistor emitter-follower circuit Butler oscillator single transistor emitter-follower schematic.svg
Single transistor emitter-follower circuit

The Butler oscillator is a crystal-controlled oscillator that uses the crystal near its series resonance point. They are used where a simple low-cost circuit is needed which can oscillate at high frquencies (>50MHz [1] ) by using overtones of a crystal, and also giving low low phase noise. [2]

Contents

It was described by Butler in 1946 as the earthed grid oscillator, a derivative of the Hartley oscillator. [3] It is also known as the bridged-T oscillator or the grounded-base oscillator. [4]

Circuit operation

The classic Butler oscillator circuit is a two-stage circuit with two non-inverting stages, a grounded base stage and an emitter follower. [5] The crystal is inserted in series in the overall feedback path. [5]

AC equivalent circuit Butler crystal oscillator-open loop AC equivalent circuit.svg
AC equivalent circuit

The more common modern form of the circuit uses just the emitter follower stage. [1] [6] The circuit may be analysed by considering it as a equivalent AC circuit with three parts. The emitter follower forms an amplifier with no phase shift. The crystal and its loading capacitor then produce a phase lag network, followed by the LC network of the resonant tank circuit. This then produces a phase lead, which overall meets the Barkhausen criteria for self-oscillation. [1]

The Butler circuit is a free-running or tuned oscillator. If the crystal is replaced temporarily with a low value resistor, the circuit will still oscillate at approximately the design frequency of the tank circuit. This allows the circuit to be set-up and adjusted initially without the crystal, and also encourages the selection of the correct crystal harmonic. [6] To avoid the circuit oscillating at the strong resonance of the crystal's fundamental, a small inductor may be placed in parallel with the crystal. [1] [6]

Both the better-known Pierce and Colpitts oscillator circuits may be considered as derivatives of the Butler. [6] [lower-roman 1]

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Microelectromechanical system oscillators are devices that generate highly stable reference frequencies to measure time. The core technologies used in MEMS oscillators have been in development since the mid-1960s, but have only been sufficiently advanced for commercial applications since 2006. MEMS oscillators incorporate MEMS resonators, which are microelectromechanical structures that define stable frequencies. MEMS clock generators are MEMS timing devices with multiple outputs for systems that need more than a single reference frequency. MEMS oscillators are a valid alternative to older, more established quartz crystal oscillators, offering better resilience against vibration and mechanical shock, and reliability with respect to temperature variation.

References

  1. In the sense of circuit analysis, rather than historical origin.
  1. 1 2 3 4 "Butler Crystal Oscillator Design" (PDF). Understanding Quartz Crystals and Oscillators. pp. 237–247.
  2. Cushing, Richard; Swift, Steven. "A Discrete, Low Phase Noise, 125 MHz Crystal Oscillator for the AD9850 Complete Direct Digital Synthesizer" (PDF). Analog Devices. AN-419.
  3. Butler, F. (June 1946). "Series-Resonant Crystal Oscillators". Wireless Engineer. 23: 157–160.
  4. Karlquist, Richard (January 1999), A New Type of Balanced-Bridge Controlled Oscillator (PDF), Hewlett-Packard, HPL-1999-6, archived from the original (PDF) on 2016-03-03 Butler, Meacham, Sultzer, ...
  5. 1 2 Gottlieb, Irving M. (1997), Practical Oscillator Handbook, Newnes, pp. 164–165, ISBN   0-7506-3102-3
  6. 1 2 3 4 "Crystal Theory" (PDF). Technical Notes. Somerset UK: EuroQuartz. Archived from the original (PDF) on 8 February 2015. Retrieved 8 February 2015.

Further reading