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Underwater Robots - Gianluca Antonelli.pdf

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196 7. Dynamic Control of UVMSs<br />

and thus only the inverse of the (6 × 6) manipulator Jacobian J m is required<br />

in the inverse kinematics algorithm.<br />

Aconstantocean currentaffect the motionwith the following components:<br />

ν I c =[0 . 1 0. 3 0 0 0 0] T m/s .<br />

As reported in [14, 13], some ofthe parameters of the controllers are related<br />

tothe knowledge ofthe mass and the first moment of gravity/buoyancy.<br />

Their initial estimate are set so as to give anestimation error larger then<br />

20% of the true values. The other parameters are related to the presence of<br />

the current. Those, will be initialized to the null value.<br />

The control law parameters have been set to:<br />

Λ 0 =blockdiag { 0 . 4 I 3 , 0 . 6 I 3 } ,<br />

Λ i =1, 6 =blockdiag { 0 . 9 I 3 , 0 . 9 I 3 } ,<br />

K v,0 =blockdiag { 9100I 3 , 9800I 3 } ,<br />

K v,i =1, 6 =blockdiag { 600I 3 , 800I 3 } ,<br />

K θ,0 =100I 9 ,<br />

K θ,i =1, 6 =40 I 9 ,<br />

where I 9 is the (9 × 9) identity matrix.<br />

The results are reported in Figures 7.31–7.32 interms of end-effector<br />

position/orientation tracking errors; it can be recognized that, in spite ofthe<br />

demanding task commanded to the system, the errors are kept small in the<br />

transients and reach zero values at steady state.<br />

e.e. position error [m]<br />

0.1<br />

0.05<br />

0<br />

−0.05<br />

y<br />

−0.1<br />

0 10 20 30<br />

time [s]<br />

Fig. 7.31. Virtual decomposition control +proper adaptive action. End-effector<br />

position error<br />

Moreover, the results inFigures 7.33–7.35 show that the control force<br />

and moments acting on the vehicle, aswell as the control torques applied<br />

z<br />

x

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