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crystals can reach only up to 20 MHz, yet can attain much higher frequencies on harmonic and/or overtone oscillator operation For example, a harmonic crystal oscillator, with its output tank circuit tuned to one of these harmonics, can have an output at the crystal s second, third, fourth, etc, harmonic, yet the crystal itself is really only operating at its lower fundamental frequency When operated as an overtone crystal oscillator, the crystal must actually vibrate at high harmonic (overtone) frequencies, and will work only at one of its odd harmonics such as its third, fifth, or seventh with the output tank circuit tuned to this chosen frequency Overtone crystal oscillators normally require a special overtone crystal when operated in this mode As stated above, the crystal functions as a very high-Q series resonant circuit with high temperature stability and very narrow bandwidth (as the highQ designation would indicate), with the crystal looking to the rest of the oscillator s circuit as shown in Fig 49 Rs is the resistance of the crystal during series resonance, while Lm is the motional inductance, Cm the motional capacitance, and C0 is the capacitance between the crystal s holder or, in a modern crystal, its plated electrodes In fact, C0 at VHF and above has so decreased in reactance that it has effectively shorted the output of the crystal to its input; this problem can be mitigated by resonating a small value coil in parallel with C0 Most oscillators will operate in series resonance mode, with the values of Lm and Cm governing the resonant frequency of the crystal At series resonance the crystal is resistive with no reactances, since XL XC, and can be described as: fs 1 2 LmCm

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As mentioned above, fundamental crystal operation usually peaks out at 20 MHz This is due not only to the dangerously decreasing thickness of the crystal, but also to its decreasing RS The crystal s RS can decrease to 10 ohms at 20 MHz on its fundamental, while the crystal in seventh overtone mode can reach 180 MHz with an RS of 80 ohms This demonstrates why many oscillators must run in overtone modes, which allow the crystal to be more easily impedance matched at higher operational frequencies Lm, whose value is based on the mechanical mass of the quartz crystal, can vary in inductance anywhere between 3600 mH at 15 MHz to 10 mH at 20 MHz Cm, whose value is based on the actual stiffness of the quartz crystal, the size of the electrodes, and the size of the quartz, can vary anywhere between 0007 pF at a fundamental frequency of 15 MHz to 002 pF at its fundamental frequency of 20 MHz But when a crystal is operated on an overtone, the Cm will decrease The designer can choose the value of the Cm desired, and the Lm will then be: Lm 1 4 frCm

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Downloaded from Digital Engineering Library @ McGraw-Hill (wwwdigitalengineeringlibrarycom) Copyright 2004 The McGraw-Hill Companies All rights reserved Any use is subject to the Terms of Use as given at the website

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