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5.3. BACKSTEPPING: MORE GENERAL CASES 145<br />

which can be accomplished by choosing<br />

leading to<br />

x2 = 0(x1) = -XI - axi<br />

21 = -xl -X 3 X.<br />

Step 2: To stabilize the original system (5.22)- (5.23), we make use of the control law<br />

(5.21). We have<br />

u<br />

8x<br />

[f (x) + g(xX] - -5X 1 g(x) - k[C - O(x)]<br />

= -(1+2axi)[ax2 i-x3 l+x2]-xl-k[x2+xl+ax2i].<br />

With this control law the origin is globally asymptotically stable (notice that Vl is radially<br />

unbounded). The composite Lyapunov function is<br />

V=Vi+2z2 = 2X2+2[x2-O(xl)]2<br />

=<br />

2X2 + 2[x2 - xl + ax T.<br />

5.3 Backstepping: More General Cases<br />

In the previous section we discussed integrator backstepping for systems with a state of the<br />

form [x, l;], x E 1R", E 1R, under the assumption that a stabilizing law 0. We now look at<br />

more general classes of systems.<br />

5.3.1 Chain of Integrators<br />

A simple but useful extension of this case is that of a "chain" of integrators, specifically a<br />

system of the form<br />

th = f(x) + g(X)1<br />

41 = 6

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