Underwater Robots - Gianluca Antonelli.pdf
Underwater Robots - Gianluca Antonelli.pdf
Underwater Robots - Gianluca Antonelli.pdf
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42 2. Modelling of <strong>Underwater</strong> <strong>Robots</strong><br />
2.9.1 Linearity inthe Parameters<br />
UVMS have aproperty that iscommon to most mechanical systems, e.g., serial<br />
chain manipulators: linearity inthe dynamic parameters. Using asuitable<br />
mathematical model for the hydrodynamic forces, (2.71) can be rewritten in<br />
amatrix form that exploits this property:<br />
Φ ( q , R I B , ζ , ˙ ζ ) θ = τ (2.73)<br />
with Φ ∈ R (6+n ) × n θ ,being n θ the total number ofparameters. Notice that n θ<br />
depends on the model used for the hydrodynamic generalized forces and joint<br />
friction terms. For asingle rigid body the number of dynamic parameter n θ,v<br />
is anumber greater than 100 [127]. For an UVMS it is n θ =(n +1) · n θ,v ,<br />
that gives an idea of the complexity ofsuch systems.<br />
Differently from ground fixed manipulators, in this case the number of<br />
parameters can not be reduced because, due tothe 6degrees of freedom<br />
(DOFs) of the sole vehicle, all the dynamic parameters provide an individual<br />
contribution to the motion.<br />
2.10 Contact with the Environment<br />
If the end effector of arobotic system is in contact with the environment,<br />
the force/moment atthe tip ofthe manipulator acts onthe whole system<br />
according to the equation ([254])<br />
M ( q ) ˙ ζ + C ( q , ζ ) ζ + D ( q , ζ ) ζ + g ( q , R I B )=τ + J T w ( q , R I B ) h e , (2.74)<br />
where J w is the Jacobian matrix defined in (2.67) and the vector h e ∈ IR 6 is<br />
defined as<br />
� �<br />
f e h e =<br />
µ e<br />
i.e., the vector of force/moments at the end effector expressed in the inertial<br />
frame. If it is assumed that only linear forces act on the end effector<br />
equation (2.74) becomes<br />
M ( q ) ˙ ζ + C ( q , ζ ) ζ + D ( q , ζ ) ζ + g ( q , R I B )=τ + J T pos( q , R I B ) f e<br />
(2.75)<br />
Contact between the manipulator and the environment is usually difficult<br />
to model. In the following the simple model constituted by africtionless and<br />
elastically compliant plane will be considered. The force at the end effector is<br />
then related to the deformation of the environmentbythe following simplified<br />
model [79] (see Figure 2.5)