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Oscillator Design



            224  Chapter Four

                        simulations predict that a reactance of 50 ohms is possible for the output
                        capacitor or inductor into the load, while still maintaining the proper gain
                        margin, then more power can safely be output into the load. Optimize this cou-
                        pling reactance value in the open-loop Bode simulations by decreasing the
                        reactance of the coupling element until the gain margin is still at a safe level
                        of at least 5 dB or greater. This also means that a true conjugate match direct-
                        ly from the oscillator output to the load input is usually impossible, since it
                        would excessively load down the oscillator, and prevent it from starting or
                        from running properly.
                          The approximate output power of the oscillator can be found in Spice by
                        employing the oscilloscope tool across the oscillator’s load and calculating:

                                     V   2                                 P
                                       RMS
                                 P         (in watts)    or    P   10 log       (in dBm)
                                       R                                 1 mW
            4.2 VCOs and LC Oscillators

            4.2.1 Introduction
                        Today, LC oscillators are normally variable frequency oscillators (VFOs) of the
                        voltage-controlled oscillator (VCO) type since they can readily be tuned by
                        adjusting the capacitance of a varactor diode to set the frequency of oscillation.
                        Still, very low cost products that utilize fixed-frequency LC oscillators can be
                        found, sometimes up to 2.4 GHz; but they have poor frequency stability over
                        temperature and poor phase-noise specifications because of their very low Q.
                          Indeed, for any LC oscillator to be even remotely frequency stable, and have
                        decent phase noise, it will require a high capacitance-to-inductance ratio in its
                        LC circuit (for a higher Q), a steady and clean power supply, stable tempera-
                        ture conditions, and strong isolation from its load. Still,  LC oscillators will
                        drift in frequency by up to 1 percent or more because of aging components or
                        (if unshielded) when a conductive surface is in close proximity. For any quality
                        wireless device this is unacceptable—unless some form of frequency regula-
                        tion is employed.
                          As mentioned above, LC oscillators are found mainly in voltage-controlled
                        oscillator circuits, since VCOs are heavily utilized in frequency synthesis for
                        phase-locked loops, and in any application where a DC control voltage is
                        required to alter the output frequency of an oscillator.


            4.2.2 Types of LC oscillators
                        There are numerous kinds of LC oscillators. However, both the Hartley and
                        the Colpitts oscillators are very common, and an understanding of their func-
                        tion will allow a good grasp of other LC designs.
                          The Hartley oscillator, as shown in Fig. 4.11, exploits a tapped coil in its tank
                        circuit, made of L and C , to change the phase of the feedback to the transis-
                                         1     1
                        tor’s base into a regenerative signal, and to set the frequency of oscillation. C
                                                                                                2

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