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212             Chapter 3  State Variable  Models

                                                         d  y     dy
                                                         J
                                              Mass  M>: M 2- j  +  b 2-j-  +  k(y  -  q)  = 0.
                                                          dt      dt
                            To  develop  the state  variable  model, we choose  the state  variables  as x\  = q and
                               =  y. Then we have
                            ,v 2
                                                          dq             dy
                                                     x-i  =  —  a n d  A'4 =  —-.
                                                          dt             dt
                            Then, in matrix  form,

                                                          x  =  Ax +  Bw,
                            and we have

                                                                 <1
                                                                  y
                                                                 q
                                                                  y
                                                                  o
                                                          B=      °
                                                                1/Afi
                                                                  0
                            and


                                                    0        0        1        0
                                                    0        0       0         1
                                           A  =                                               (3.119)
                                                  -klM x                       0
                                                                     0
                                                  k/M 2   -k/M 2            ~b 2/M 2
                            Note  that  the  output  is  y(t)  = x 4.  Also,  for  L  =  0 or  negligible  inductance,  then
                            u(t)  =  K mv(t).  For the typical parameters and for k  =  10, we have

                                                                  0
                                                                  0
                                                            B  =
                                                                 50
                                                                  0_
                            and
                                                      0        0        1     0
                                                      0        0       0       1
                                             A  =
                                                     -500     +500    -20.5   0
                                                    +20000   -20 000   0     -8.2
                            The response  of y for u(t)  =  1, t  >  0 is shown in Figure  3.42. This response is quite
                            oscillatory, and it is clear that we want a very rigid flexure with k  > 100.
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