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NONLINEAR CONTROLLER COMPARISON ON A BENCHMARK ...

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control Lyapunov function globally asymptotically stable. Backstepping essentially<br />

tries to reduce the system to a number of subsystems in series. Then the stabilizing<br />

inputs for the subsystem closest to the output are computed, and these inputs are<br />

then treated as the outputs of the previous system, and a new set of inputs to this<br />

next subsystem are computed to guarantee stability. This process is repeated until<br />

the original control input is computed. Control laws generated by this methodol-<br />

ogy, as shown in [1], are proven to stabilize the system globally and asymptotically.<br />

However, this design procedure is the most di cult to compute and implement, and<br />

the resulting control law is both complicated and cumbersome. The rst step is<br />

to apply a variable transformation to the exible beam's non-dimensionalized state<br />

equations (2.5) to obtain:<br />

z 1 = x 1 + sin( )<br />

z 2 = x 2 + _ cos( )<br />

y 1 = x 3<br />

y 2 = x 4<br />

v =<br />

1<br />

1 ; 2 cos 2 ( )<br />

cos( )(z1 ; (1 + _2 ) sin( )) + k2 mk2 g<br />

Rmmc (z2 ; _ cos( )) + kmkgu<br />

R ; m<br />

(3.18)<br />

This variable substitution and the feedback transformation from u to v (which is<br />

a non-singular transformation because the parameter is always smaller than 1)<br />

simpli ed the system equations to the following form:<br />

z_ 1 = z2 z_ 2 = ;z1 + sin( )<br />

y_ 3 = _<br />

y_ 4 = = v<br />

22<br />

(3.19)

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