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Underwater Robots - Gianluca Antonelli.pdf

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62 3. Dynamic Control of 6-DOF AUVs<br />

desired orientation [deg]<br />

100<br />

80<br />

60<br />

40<br />

20<br />

0<br />

φ<br />

θ<br />

−20<br />

0 100 200<br />

time [s]<br />

300 400<br />

Fig. 3.3. Desired trajectory; the desired position is constant<br />

Table 3.3. Initial conditions for all the controllers in their reduced version and<br />

number of parameter to adapt/integrate<br />

law number ofpar. ˆ θ ( t =0)<br />

A 7 [0 0 0 0 0 0 1] T (initial value of the integral)<br />

B – not simulated<br />

C 10 [ − 9 0 50 0 0 0 0 0 0 0] T<br />

D 10 [ − 9 0 50 0 0 0 0 0 0 0] T<br />

E 9 [0 50 0 0 0 9 0 0 0] T<br />

F 9 [0 50 0 0 0 9 0 0 0] T<br />

Ocean current The simulations have been run considering the following<br />

constant current<br />

ν I c =[0 0. 3 0 0 0 0] T m/s ,<br />

Gains selection All the simulated controllers are non-linear. Moreover, significant<br />

differences arise among them, this is, in fact, the object of this discussion.<br />

For these reasons it is very difficult toperform afair numerical<br />

comparison and the selection of the gains is very delicate. The gains have<br />

been tuned so as to give tothe controller similar control effort interms of<br />

force/moment magnitude and eventual presence ofchattering. Infew cases,<br />

since the controller feeds back the same variable, ithas been possible to chose<br />

the same control gain, itisthe case, e.g., of the controllers C and E .Inother<br />

cases, such as, e.g., the controller F ,the use of the transpose of the Jacobian<br />

ψ

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