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104             Chapter 2  Mathematical  Models of Systems

                               1.04

                               1.03


                               1.02


                               1.01





                               0.99


                              0.98
           FIGURE 2.43
           The water level
           response to a       0.97
           sinusoidal variation            200        400       600       800        1000
           in the input flow.                            Time (s)


                           Thus in the steady-state  (see Figure 2.42) we expect that the output flow rate will os-
                           cillate at a frequency  of at —  0.05 rad/s, with a maximum value of

                                             Qo   =Q*  +  |AQ 2(0l max  =  35.18 kg/s.  •


                           EXAMPLE 2.14     Electric traction motor control
                           A  majority  of modern  trains  and  local transit  vehicles utilize  electric traction  mo-
                           tors. The electric motor drive for a railway vehicle is shown in block diagram form in
                           Figure 2.44(a), incorporating the necessary control of the velocity of the vehicle. The
                           goal of the design is to obtain a system model and the closed-loop transfer  function
                           of the  system, a)(s)/a) d(s),  select  appropriate  resistors  R h  R 2, R$, and  R A, and  then
                           predict the system response.
                               The first  step is to describe the transfer  function  of each block. We propose  the
                           use  of  a tachometer  to generate  a voltage proportional  to velocity and  to connect
                           that  voltage, v u  to one  input  of  a difference  amplifier,  as shown  in Figure  2.44(b).
                           The  power  amplifier  is  nonlinear  and  can  be  approximately  represented  by
                                  2vx
                           v 2  =  2e  = g(vi),  an  exponential  function  with  a  normal  operating  point,
                           v w  =  1.5 V. Using the technique  in Section 2.3, we then obtain a linear model:

                                  dgM
                           Ai>>  =        Av y  =  2[3 exp(3w 10)] A^  =  2(270) A^  =  540 A^.   (2.126)
                                   dvi
                                        «10
                           Then, discarding the delta notation and using the Laplace transform, we find  that

                                                       V 2(s)  =  StoV^s).
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