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Nonlinear Control Sy.. - Free

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Chapter 3<br />

Lyapunov Stability I: Autonomous<br />

<strong>Sy</strong>stems<br />

In this chapter we look at the important notion of stability in the sense of Lyapunov.<br />

Indeed, there are many definitions of stability of systems. In all cases the idea is: given a<br />

set of dynamical equations that represent a physical system, try to determine whether such<br />

a system is well behaved in some conceivable sense. Exactly what constitutes a meaningful<br />

notion of good behavior is certainly a very debatable topic. The problem lies in how to<br />

convert the intuitive notion a good behavior into a precise mathematical definition that can<br />

be applied to a given dynamical system. In this chapter, we explore the notion of stability<br />

in the sense of Lyapunov, which applies to equilibrium points. Other notions of stability<br />

will be explored in Chapters 6 and 7. Throughout this chapter we restrict our attention to<br />

autonomous systems. The more general case of nonautonomous systems is treated in the<br />

next chapter.<br />

3.1 Definitions<br />

Consider the autonomous systems<br />

x=f(x) f:D -Rn<br />

where D is an open and connected subset of Rn and f is a locally Lipschitz map from D<br />

into Rn. In the sequel we will assume that x = xe is an equilibrium point of (3.1). In other<br />

words, xe is such that<br />

f(xe) = 0.<br />

'Notice that (3.1) represents an unforced system<br />

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