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Reflections of a Dinosaur


                vcc  l+15  Volts1
                             7"
                                             Eight
               Rl                           Equally
              12 K                         Weighted

                     N
                                     CR2
                          MSB
            lout*-
                                   :+\
                       R15
                      1.0  K
                                R16
                              1.0  K

                Figure 6-5.
           Transistor-diode
                 switched   the outputs of the current steering switches. For those unfamiliar with the R-2R
           individual current   ladder, it is an interesting exercise to calculate what fraction of current introduced
              division 12-bit   into the nth R-2R-R node will reach a load resistor RL connected from the IOut node
                    DAC.   to ground. A little mathematical manipulation will show that the current introduced
                          at any node of the R-2R ladder is attenuated by
                             2-"  X (2R/(RL+2R))
                           when it reaches the load resistor RL; where n = the number of stages between the
                           node where the current is introduced and the lout node.
                             n = 0 for the MSB
                             n = 1 for the MSB-1
                             n = 2 for the MSB-2




                             n = n - 2 for the LSB+I
                             n = n - 1 for the LSB
                           An interesting property of the R-2R ladder is that the resistance of the ladder at any
                          R-2R node looking to the right is always 2R. Using Figure 6-4 as an example, the
                          resistance looking into R35 is 1000 (n, R35 + R36. The resistance looking into R33
                           is also 1000 {I, (R33 added to the parallel combination of R34 with the sum of R35
                           and R36). This calculation can be repeated at each node, and you will find that the
                           resistance looking into IOU[ is also 2R.
                             When all the current sources are made equal and the current division is done with
                           the R-2R ladder, the switching times of each bit are matched. The physical length of
                           the R-2R ladder will introduce a differential delay from each bit to the Z,,,,  node, but
                           this is a very small effect and turns out not to be important if the resistance of the
                           R-2R ladder is low. Even the small delay due to the propagation time through the
                          R-2R ladder can be reduced by providing a separate divider for each bit (see Figure
                           6-5). This scheme has been tried, and the results are almost identical to the dynamic
                          performance of the R-2R divider.
                             The use of equal current sources and a resistive divider, either the R-2R or the
                           individual, improves the dynamic performance. The improved performance is gained
                           at the expense of complexity and power consumption. The R-2R and the individual
                          divider circuits use three resistors per bit instead of the one resistor per bit of the

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