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168    ACCOUNTING FOR BODY DYNAMICS: THE JOGGER’S PROBLEM

                           x
                                                      Switch  h
                                                      curve
                                      Start
                                      position

            Point of
            switching
                                           dx                               dh
                                           dt                                dt
                                                      Final
                     Final                            position
                     position                                          Point of
                                                                       switching
                                                     Start
                                                     position
                              Switch
                              curve
           Figure 4.9  (a) The start position in the phase space (ξ, ˙ ξ) is above the switch curves.
           (b) The start position in the phase space (η, ˙η) is under the switch curves.


           switch curves. For example, if the initial conditions for ξ and η are as shown in
           Figure 4.9, then

                                       −p max , 0 ≤ t ≤ t s,ξ
                                ˆ p(t) =
                                       +p max ,t s,ξ <t ≤ t f

                                       +q max , 0 ≤ t ≤ t s,η
                               ˆ q(t) =                                  (4.19)
                                       −q max ,t s,η <t ≤ t f
           where the caret sign (ˆ) refers to the parameters under optimal control. The
           time, position, and velocity of the control switching for the ξ components are
           described by


                                         ( ˙ ξ 0 ) 2   ˙
                                          2  + ξ 0 p max + ξ 0
                                 t s,ξ =
                                              p max
                                        ξ ˙ 2 0  ξ 0
                                  ξ s =     +
                                       4p max  2

                                            ξ ˙ 2
                                  ˙
                                  ξ s =−    0   + ξ 0 p max
                                          2p max
           and those for the η components are described by


                                         (˙η 0 ) 2
                                             − η 0 q max −˙η 0
                                          2
                                 t s,η =
                                              q max
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