Page 73 - Human Inspired Dexterity in Robotic Manipulation
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Modeling and Human Performance in Manipulating Parallel Flexible Objects  69


                                1            1
                                          2
                          ω 2  ¼ ð1+ μ Þω + ð1+ μ Þω   2
                                                    2
                           1,2
                                       1
                                2         1  2         2
                             s  ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
                                                                             2
                                                   1         2  1         2
                                   2
                                 2
                              ω ω ð1+ μ + μ Þ +      ð1+ μ Þω + ð1+ μ Þω  2  ,
                                 1
                                              2
                                                          1
                                          1
                                   2
                                                                       2
                                                             1
                                                   2            2
                                                                         (5.29)
              where
                                          m 1         m 2
                                   μ 1  ¼   , μ 2  ¼    :                (5.30)
                                          m h         m h
                 Note that matrix A in Eq. (5.37) is not in block upper triangular form as
              in Eq. (5.11). To facilitate the computations, define the center of mass
                                       m h x h + m 1 x 1 + m 2 x 2
                                   x c ¼                                 (5.31)
                                          m h + m 1 + m 2
              and rearrange the system dynamics (5.5), (5.26)as
                                     2
                                             2
                                                                2
                         € x 1 + ð1+ μ Þω x 1 + μ ω x 2 ¼ð1+ μ + μ Þω x c ,  (5.32)
                                  1  1     2  1          1   2  1
                                                                2
                                     2
                                             2
                         € x 2 + ð1+ μ Þω x 2 + μ ω x 1 ¼ð1+ μ + μ Þω x c ,  (5.33)
                                                         1
                                           1
                                                             2
                                  2
                                     2
                                             2
                                                                2
                                         € x x ¼ F=M,                    (5.34)
              where M ¼ m h + m 1 + m 2 is the total mass. With the state vector
                                                        T
                                   x ¼ x 1 , _x 1 ,x 2 , _x 2 ,x c , _x c ,F½  Š  (5.35)
              and control u ¼ _ F, the state dynamics
                                         _ x ¼ A + bu                    (5.36)
              have the block upper triangular form
                   0           1      0      0       0       0   0         0
                  2                                                 3     2 3
                    ð1+ μ Þω 2  0   μ ω 2    0 ð1+ μ + μ Þω 2  0
                  6       1  1        2 1           1   2  1     0 7      6  07
                  6                                                 7     6 7
                   0           0      0      1       0       0
                  6                                              0 7      6  0 7
                                                                          6 7
                  6
              A ¼  μ ω  2      0  ð1+ μ Þω 2  0 ð1+ μ + μ Þω 2  0  0  7 , b ¼ 0 :
                                                        2
                                                                    7
                                                                          6 7
                  6
                      1 2
                                        2
                                                    1
                  6                        2               2        7     6 7
                   0           0      0      0       0       1   0         0
                  6                                                 7     6 7
                  6                                                 7     6 7
                   0           0      0      0       0       0 1=M         0
                  4                                                 5     4 5
                   0           0      0      0       0       0   0         1
                                                                         (5.37)
                 The minimum hand-force-change model can now be stated as the fol-
              lowing optimization problem with fixed end-points: Minimize the
              minimum-effort-type criterion
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