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Nonlinear Control Sy.. - Free

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266 CHAPTER 10. FEEDBACK LINEARIZATION<br />

1- The feedback law (10.4) was obtained with the sole purpose of linearizing the original<br />

state equation. The resulting linear time-invariant system may or may not have<br />

"desirable" properties. Indeed, the resulting system may or may not be stable, and<br />

may or may not behave as required by the particular design.<br />

2- Once a linear system is obtained, a secondary control law can be applied to stabilize<br />

the resulting system, or to impose any desirable performance. This secondary law,<br />

however, is designed using the resulting linear time-invariant system, thus taking<br />

advantage of the very powerful and much simpler techniques available for control<br />

design of linear systems.<br />

Example 10.8 First consider the nonlinear mass-spring system of example 1.2<br />

I xl = x2<br />

which can be written in the form<br />

(l x2 = mxl - ma2xi mx2 +<br />

Clearly, this system is of the form (10.3) with w = 1 and O(x) = ka2xi. It then follows that<br />

the linearizing control law is<br />

u = ka2xi + v<br />

Example 10.9 Now consider the system<br />

1 it = x2<br />

ll x2 = -axl + bx2 + cOS xl (u - x2)<br />

Once again, this system is of the form (10.3) with w = cos xl and O(x) = x2. Substituting<br />

into (10.4), we obtain the linearizing control law:<br />

u=x2+cos-l X1 V<br />

which is well defined for - z < xl < z . El

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