Page 202 - Op Amps Design, Applications, and Troubleshooting
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Voltage-Controlled Oscillator  185









        where I is the input current computed and t is the time Q is allowed to charge,
        This equation can be transposed to produce another very useful form:








        This allows us to compute the amount of time it takes Q to charge to a given volt-
        age change (AV Cl) when a given value of charging current is applied.
             We already know from earlier discussions that the limits of Q's charge are
        set by the upper and lower thresholds of A^ That is, Q will charge linearly
        between the Vjj and V UT values established by A 2. In the present circuit, the
        change in C\ voltage in going from the V LT to the V^ is






        More specifically,

                            AV Cl = 46.8 V - (-6.8 V) = 13.6 V


        If we now compute the time it takes Cj to make this voltage change, we will know
        the time for one alternation (negative slope) of the oscillator's output. Let us com-
        pute this time for input voltages of +1 and +5 volts, which were previously shown
        to produce 50 microamperes and 250 microamperes, respectively. Equation (4.12)
        gives us













        The remaining alternation (positive ramp) occurs when D 4 is forward-biased. This
        effectively connects the output of A 3 to AI via R 4. Recall that during this portion of
        the cycle, the output of A 3 is 0.6 volts larger than + V^ and is of the opposite polar-
        ity. Since diode D 4 drops 0.6 volte when it is forward-biased, this means that the
        voltage applied to the right end of Rj is exactly the same as the value of +V m, but
        it is negative instead of positive. That is, this input to AI ranges from -1 to -5 volts.
        The resulting input current through #4 is computed as
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