Page 205 - Op Amps Design, Applications, and Troubleshooting
P. 205

188    OSCILLATORS


               amperes for the 1N5226 diodes. The design value of the zener current is then com-
               puted, as in Equation (4.17):




               The value of R 2 can now be computed, as in Equation (4.18):






                    We will select a standard value of 3.6 kilohms for R 2. However, because this
               design method inherently uses a zener current that is less than the test current
               (I ZT), we can expect the regulated voltage to be less than the stated value.
               Appendix 5 includes a graph that allows us to estimate the error. In the present
               case, the zeners will have about 2.65 volts instead of the rated 3.3 volts, which
               will in turn cause the ramp output to have an amplitude of 6.5 volts instead of
               the design goal of 8. If this is an important circuit parameter for a given applica-
               tion, we should select a zener with a higher voltage rating but continue to oper-
               ate it below its rated current. We continue with our present selection, since the
               reduced voltage is still within the tolerance stated as part of the original design
               goals.

               Compute RI and Cj. Once the zeners have been selected, the values of R^ and
               Q determine the frequency for a given voltage. The required RiQ product can be
               found with Equation (4.19):









               where V MMp is the amplitude of the ramp output voltage, y w(max) is the highest
               input voltage, and/ HJ is the highest frequency of oscillation. Calculations for our
               present design example are






               At this point, we can either select Q and calculate Rj or vice versa. In either case,
               we want RI to be in the range of 1.0 to 470 kilohms, if practical. Similarly, Q
               should be greater than 470 pF and nonpolarized. Because it is essential that R 4 be
               exactly one-half the value of R\ f and because there are a limited number of resis-
               tor pairs that have exactly a 2:1 ratio, it is generally easier to select R l and com-
               pute Q.
                    For purposes of this design, let us select RI as 2 kilohms. We can then com-
               pute Q by transposing the results of Equation (4.19):
   200   201   202   203   204   205   206   207   208   209   210