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Simulation
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Simulation Results | |
Figure 13 Stable Trajectory of lo_hipK solution Figure 14 |
The following results compare two solutions for X:
For both results, the model was simulated and allowed to run until a stable trajectory was achieved. This stable cycle was used to compare with the original kinematic data. Finally, a disturbance was added to the simulation (results below). |
Overlay Movies | |
Figure 15 Overlay for lo_hipK (movie) Figure 16 |
Figures 15 and 16 show the kinematic data and the simulation results for both optimization solutions.
As can be seen, both trajectories are qualitatively similar. The trajectory for hi_hipK appears to be out of phase. |
Trajectory Comparison | |
Figure 17 X position for simulated trajectory of lo_hipK Figure 18 Figure 19 Figure 20 Figure 21 Figure 22 |
These figures compare the kinematic data with one stride period of the simulations (taken after the simulation has converged to a stable trajectory).
As seen in the figures, the results for lo_hipK appear to match the position trajectories slightly better than the results for hi_hipK. In particular, note that the simulation for hi_hipK in the X direction is out of phase with the kinematic data. Note that the kinematic data is not regular (non-cyclic), while the simulation results return to the same state at the end of the stride period. |
Disturbance Rejection Movies | |
Figure 23 Disturbance rejection for lo_hipK Figure 24 |
For both solutions, the model was simulated and a large disturbance was introduced during the simulation. The disturbance consisted of the addition of a velocity in the x direction of 1m/s.
Figures 23 and 24 show the resulting motion. As seen from the movies, the solution for hi_hipK is more robust to the disturbance. The solution for lo_hipK takes about three of four stride cycles to converge back to the particular direction. |