Page 110 - The Art and Science of Analog Circuit Design
P. 110

William H, Gross




                                                                           Figure 8-7.
                                                                           Block diagram of
                                                                           the control circuit.




                                                                     BIAS



















           The block diagram of Figure 8-7 became the circuit of Figure 8-8
        after several iterations. The common mode range of the simple op amp
        includes the negative supply and the circuit has sufficient gain for the job.
        Small current sharing resistors, Rl, R2, R3, and R4, were added to im-
        prove the high current matching of the two output currents and eliminate
        the need for the two R c resistors. The small resistors were scaled so they
        could be used for short circuit protection with Q5 and Q6 as well.
           Mirror #1 is a "super diode" connection that reduces base current errors
        by beta; the diode matches the collector emitter voltages of the matched
        transistors. Identical mirrors were used for #2 and #3 so that any errors
        would ratio out. Since these mirrors feed the emitters of the pre-distortion
        cascodes Ql and Q2, their output impedance is not critical and they are
        not cascoded. This allows the bias voltage at the base of Ql and Q2 to be
        only two diode drops below the supply, maximizing the common mode
        range of the input stages.
           While evaluating the full circuit, I noticed that when one input was
        supposed to be off, its input signal would leak through to the output. The
        level increased with frequency, as though it was due to capacitive feed-
        through. The beauty of SPICE came in handy now. I replaced the current
        steering transistors with ideal devices and still had the problem. Slowly
        I came to the realization that the feedthrough at the output was coming
        from the feedback resistor. In a current feedback amplifier, the inverting
        input is driven from the non-inverting input by a buffer amp and therefore
        the input signal is always present at the inverting input. Therefore the
        amount of signal at the output is just the ratio of the feedback resistor to
        the amplifier output impedance. Of course the output impedance rises
        with frequency because of the single pole compensation necessary to keep

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