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Underwater Robots - Gianluca Antonelli.pdf

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3.9 Numerical Comparison Among the Reduced Controllers 75<br />

However, to better illustrate this different behavior, asecond simulation<br />

study was developed in which the vehicle is commanded to c hange the sole<br />

roll angle according to the time law inFigure 3.16 while keeping constant the<br />

vehicle position and the other vehicle angles atzero; for the sake ofclarity,<br />

it is assumed that no ocean current isacting on the vehicle. The behavior<br />

of the reduced version of control law E is compared to that of the reduced<br />

version of the control law A in terms of the measured roll angles (Figure 3.17,<br />

left column). Remarkably, inthe simple condition considered, the restoring<br />

moment to be compensated for is mainly acting around the x b axis. In the<br />

simulation, it is possible to compute the restoring moment around this axis<br />

and compare it with the adaptive compensation of the control law E and the<br />

integral compensation plus the model-basedcompensation of thecontroller A<br />

respectively; those plots are reported in the rightcolumn of Figure 3.17. It can<br />

be observed that during the phase in which the roll angle changes from +10 ◦<br />

to − 10 ◦ the compensation built by the control law A has alag with respect<br />

to the acting restoring moment; this is due to the integral charge/discharge<br />

time required tobuild atime-varying compensation term. The control law E ,<br />

instead, performs proper compensation of the restoring moment since it accounts<br />

for the vehicle orientation in the adaptation mechanism.<br />

desired orientation [deg]<br />

20<br />

10<br />

0<br />

−10<br />

roll<br />

−20<br />

0 50 100 150<br />

time [s]<br />

Fig. 3.16. Comparison of the control law A and the control law E in the second<br />

case study: Time history of the desired orientation

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