overview
intro
data
model
optimization
simulation
hybrid_1
hybrid_2
conclusions

Simulation
Simulation Results
Figure 13
Stable Trajectory of lo_hipK solution

Figure 14
Stable Trajectory of hi_hipK solution

The following results compare two solutions for X:
  • simulation results for lo_hipK after 100 iterations (Figure 13)
  • simulation results for hi_hipK after 600 iterations (Figure 14)

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
Overlay for hi_hipK (movie)

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
Y position for simulated trajectory of lo_hipK

Figure 19
Orientation for simulated trajectory of lo_hipK

Figure 20
X position for simulated trajectory of hi_hipK

Figure 21
Y position for simulated trajectory of hi_hipK

Figure 22
Orientation for simulated trajectory of hi_hipK

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
Disturbance rejection for hi_hipK

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.