NONLINEAR CONTROLLER COMPARISON ON A BENCHMARK ...

NONLINEAR CONTROLLER COMPARISON ON A BENCHMARK ... NONLINEAR CONTROLLER COMPARISON ON A BENCHMARK ...

24.08.2013 Views

Response in cm 4 3 2 1 0 −1 −2 −3 Linearized Robust Linearized Optimal −4 0 1 2 3 4 5 Time 6 7 8 9 10 Figure 4.5: Linear H1 vs. Linearized Optimal than this approach in the simulations. Figures 4.7 and 4.8 show that the linearized designs attenuated the vibrations faster. A possible explanation for the strange envelope of the rst state's oscillations, is that the dynamics in the feedback loop act as an energy shaping block. It is possible that, similar to the way the energy in two coupled pendulums is transfered back and forth before damping out, energy is being coupled back and forth between the control and the system dynamics, while being steadily absorbed by the controller's virtual damping e ect. 4.2.4 Backstepping Algorithm The backstepping control design performed very well { it seemed to damp the oscillations quicker than any of the other designs in simulation. Figures 4.10 through 4.12 show that it attenuated the vibrations faster than the other control designs. There were, however, two anomalies associated with this controller: it ex- pended a great deal more control e ort than the previous designs, and it began by 34

Response in cm Response in cm 4 3 2 1 0 −1 −2 −3 Passivity Based Open Loop Response −4 0 1 2 3 4 5 Time 6 7 8 9 10 4 3 2 1 0 −1 −2 −3 Figure 4.6: Passivity Based Control vs. Open Loop Response Passivity Based Linearized Optimal −4 0 1 2 3 4 5 Time 6 7 8 9 10 Figure 4.7: Passivity Based Control vs. Linear Optimal Control 35

Response in cm<br />

4<br />

3<br />

2<br />

1<br />

0<br />

−1<br />

−2<br />

−3<br />

Linearized Robust<br />

Linearized Optimal<br />

−4<br />

0 1 2 3 4 5<br />

Time<br />

6 7 8 9 10<br />

Figure 4.5: Linear H1 vs. Linearized Optimal<br />

than this approach in the simulations. Figures 4.7 and 4.8 show that the linearized<br />

designs attenuated the vibrations faster.<br />

A possible explanation for the strange envelope of the rst state's oscillations,<br />

is that the dynamics in the feedback loop act as an energy shaping block. It is possible<br />

that, similar to the way the energy in two coupled pendulums is transfered back and<br />

forth before damping out, energy is being coupled back and forth between the control<br />

and the system dynamics, while being steadily absorbed by the controller's virtual<br />

damping e ect.<br />

4.2.4 Backstepping Algorithm<br />

The backstepping control design performed very well { it seemed to damp<br />

the oscillations quicker than any of the other designs in simulation. Figures 4.10<br />

through 4.12 show that it attenuated the vibrations faster than the other control<br />

designs. There were, however, two anomalies associated with this controller: it ex-<br />

pended a great deal more control e ort than the previous designs, and it began by<br />

34

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