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Amplifier Design



                                                                               Amplifier Design  197






















                                                      Figure 3.102 A negative
                                                      feedback circuit.



                        be found empirically (50 to 500 ohms will be the normally employed value).
                        The inductor (L) is the important component that actually controls the feed-
                        back. It functions by having a very high reactance to the amplifier’s desired
                        frequencies, so it will not permit degenerative feedback that would lower the
                        gain levels at these higher frequencies. However, as the frequency is
                        decreased, the reactance of the inductor will, of course, decrease. This
                        increases the level of degenerative feedback to the base, decreasing the gain of
                        any low-frequency signals. Feedback of any kind may sound dangerous, but a
                        common emitter amplifier will have a perfect 180 degree phase shift at its low-
                        er frequencies of operation ( f ), thus assuring that regenerative, or oscillato-
                                                     T
                        ry, feedback will not occur. The only caution would be to confirm that the
                        inductor is capable of blocking the RF at its highest frequency, and not allow
                        the RF to pass through because of parasitic capacitances within this choke.
                          But if we keep in mind that almost any amplifier will be completely stable
                        if all of the frequencies it is passing can see a perfect 50-ohm resistive imped-
                        ance at both its input and output (a difficult objective with power amplifiers),
                        then we can use this knowledge to our advantage. Excellent stability—even at
                        frequencies above or below our interests—can be assured by supplying the
                        transistor with a good 50-ohm source and load. This can be in the form of a 51-
                        ohm load resistor that will be seen only by the unnecessary lower frequencies
                        through a one-pole low-pass filter, or by the use of a diplexer, or by employing
                        a 1- or 2-dB 50-ohm pad at the amplifier’s output.
                          Another viable technique to design stable wideband amplifiers is by using
                        resistive components to match an amplifier over its entire bandwidth (Fig.
                        3.103). However, this technique has a large disadvantage of producing much
                        lower gain compared to the typical LC matching method, with less reverse iso-
                        lation and a higher noise figure. Its greatest advantage is that it has a very



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