Page 438 - Op Amps Design, Applications, and Troubleshooting
P. 438

414     SPECIALIZED DEVICES


               where k is a constant determined by the circuit configuration. Substitution of this
                latter equation into the preceding equation gives us a form that reveals the multi-
                plier action of the multiplier circuit.




                Here we can see that the output voltage is clearly a result of multiplying the input
                voltages together with a circuit constant. The value of the constant (k) is typically
                0.1.
                    Since each of the input voltages may take on either of two polarities, this
               leads to four possible modes of operation. These four modes, or quadrants, are
               illustrated in Figure 11.7.
                    If a particular multiplier circuit is designed to accept only one polarity of
               input voltage on each of its inputs, then its operation will be limited to a single
               quadrant and it will be called a one-quadrant multiplier. Similarly, if a given multi-
               plier circuit requires a single polarity on one input but accepts both polarities on
               the other, the device is called a two-quadrant multiplier. Finally, if a multiplier is
               designed to accept either polarity on both of its inputs, then the device is called a
               four-quadrant multiplier. The AD532 is a four-quadrant multiplier—it will accept
               voltages as large as ±10 volts on its inputs and produces output voltages as large
               as ±10 volts. The AD532 employs differential inputs and generates a single-ended
               output voltage described by the following expression:






               Figure 11.8 shows the schematic diagram of an AD532 circuit connected as a sim-
               ple multiplier. The oscilloscope display in Figure 11.9 indicates the actual behavior
               of the circuit.
                    In Figure 11.9, waveforms 1 and 2 are the input signals. Waveform 4 is the
               output of the multiplier circuit, and, again, its operation is easily understood by
               viewing it as a variable gain amplifier. One input (e.g., channel 1 in Figure 11.9)
               controls the gain for the second input (e.g., channel 2 in Figure 11.9).
















        FIGURE 11.7 There are four possible
        modes or quadrants of operation for
        multiplier circuits.
   433   434   435   436   437   438   439   440   441   442   443