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with higher transistor bias current we can also decrease the phase noise, since the carrier will now be at a higher relative amplitude above this noise As open-loop oscillator design accuracy depends on both ends of the oscillator loop being at the same impedance (as well as both terminating impedances in the linear simulator being equal), then it can be seen that ignoring cascaded input and output impedances will result in a nonoptimized oscillator design However, a new technique that allows the oscillator designer to not have so much dependence on the oscillator s terminating impedances with the linear simulator for an accurate prediction of the oscillator s gain and phase has just been recently presented This new technique employs Harada s equations, and assumes that S12 equals zero, which is never the case Therefore, it is recommended that for ease of computations, and for very acceptable accuracy, that normal open-loop analysis (as demonstrated by Rhea) should be followed for the design of most oscillators In utilizing open-loop oscillator design, it is assumed that the open loop is stable In other words, the amplifier section (with bias) should not be unstable, since it is only when the loop is closed from input to output that oscillations are meant to occur Proper frequency stability may become quite erratic with an unstable device, so choose only unconditionally stable transistors When simulating a crystal oscillator, we must first select the proper crystal by obtaining certain crystal parameters (Fig 49), such as the crystal s motional capacitance (CM), motional inductance (LM), series resistance (RM), and parallel plate capacitance (CP or C0) from the manufacturer for the crystal s desired frequency of operation, its holder type, and quartz cut (typically AT) The manufacturer will also need to be informed if the crystal is to be utilized in a series or parallel resonance oscillator (see Pierce Crystal Oscillator Design in Sec 433), and whether the crystal is being run on its fundamental or on one of its overtone frequencies The crystal s required aging specification in parts per million per year (ppm/year), initial frequency accuracy in ppm, and the frequency accuracy over temperature in ppm are all important as well Since many linear computer simulation packages may not necessarily have crystal models available, we must model the crystal as shown in Fig 49, and place it where the crystal would be within the oscillator circuit This equivalent LCR model, while simplistic, is more than adequate to realistically repre-.

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