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A New  Do11ain  and  More  Process  Models   107



        4-5  A First-Order with Dead-Time (FOWDT) Process
             Consider Fig. 4-33 where the tank of liquid has been placed upstream of
             the pure dead-time process. The placement of the buckets-on-the-belt
             ahead of the tank suggests a dead time in series with a first-order pro-
             cess. Please do not be confused by the length of the pipe at the outlet of
             the tank. Let's assume that it  is actually relatively short and that the pipe
             diameter is small so that the transit time of  the liquid spent in the pipe is
             negligible compared to the time spent in the buckets on the belt
                Figure 4-34 shows the open-loop step-change response of the pro-
             cess for the case of g = 2.5, -r= 10, D = 8. This is the first example pro-
             cess in this chapter that has had a nonunity gain.
                In the continuous time domain, this model would be described
             by an extension of the first-order model:

                               -r~~  +y=gU(t-D)                 (4-16)

                In the Laplace domain, the open-loop transfer function is
                                G (s) =  e-sD_g_                (4-17)
                                 P        t'S+ 1
                After applying s =  jro, the magnitude and phase can be found as
             follows:
                           G
                             (jro) =  e-it»D -.  _g_  =  IG lei'
                             p         ]t'OJ+ 1   p

                              I GI-   g                         (4-18)
                                P- J<-rrof + 1
                                       1
                                8=  -tan- (-rro)- roD

                        Valve position (U)
                             J;
                    I

                    '












             F1auRE 4-33  First-order process with dead time.
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