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Nonlinear Control Sy.. - Free

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10.2. INPUT-STATE LINEARIZATION 265<br />

and thus<br />

223 -21 -4X3<br />

fl f2 [fl, f2] 1 = -1 -2X2 2<br />

0 X3 0<br />

which has rank 2 for all x E R3. It follows that the distribution is involutive, and thus it is<br />

completely integrable on D, by the Frobenius theorem.<br />

10.2 Input-State Linearization<br />

Throughout this section we consider a dynamical systems of the form<br />

± = f(2) + g(x)u<br />

and investigate the possibility of using a state feedback control law plus a coordinate<br />

transformation to transform this system into one that is linear time-invariant. We will<br />

see that not every system can be transformed by this technique. To grasp the idea, we start<br />

our presentation with a very special class of systems for which an input-state linearization<br />

law is straightforward to find. For simplicity, we will restrict our presentation to single-input<br />

systems.<br />

10.2.1 <strong>Sy</strong>stems of the Form t = Ax + Bw(2) [u - cb(2)]<br />

First consider a nonlinear system of the form<br />

2 = Ax + Bw(2) [u - q5(2)] (10.3)<br />

where A E Ilt"', B E II2ii1, 0 : D C II2" -4 )LP1, w : D C 1(P" -4 R. We also assume that<br />

w # 0 d2 E D, and that the pair (A, B) is controllable. Under these conditions, it is<br />

straightforward to see that the control law<br />

renders the system<br />

u = O(2) + w-1 (2)v (10.4)<br />

i=A2+Bv<br />

which is linear time-invariant and controllable.<br />

The beauty of this approach is that it splits the feedback effort into two components<br />

that have very different purpose.

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