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256 CHAPTER 10. FEEDBACK LINEARIZATION<br />

is a function f : D C R" -> 1R1, namely, a mapping that assigns an n-dimensional vector<br />

to every point in the n-dimensional space. Defined in this way, a vector field is an<br />

n-dimensional "column." It is customary to label covector field to the transpose of a vector<br />

field. Throughout this chapter we will assume that all functions encountered are sufficiently<br />

smooth, that is, they have continuous partial derivatives of any required order.<br />

10.1.1 Lie Derivative<br />

When dealing with stability in the sense of Lyapunov we made frequent use of the notion<br />

of "time derivative of a scalar function V along the trajectories of a system d = f (x)." As<br />

we well know, given V : D -+ 1R and f (x), we have<br />

f (x) = VV f (x) = LfV(x).<br />

x<br />

A slightly more abstract definition leads to the concept of Lie derivative.<br />

Definition 10.1 Consider a scalar function h : D C 1R" -* JR and a vector field f : D C<br />

]R" -4 1R" The Lie derivative of h with respect to f, denoted Lfh, is given by<br />

Lfh(x) = ax f (x). (10.1)<br />

Thus, going back to Lyapunov functions, V is merely the Lie derivative of V with respect<br />

to f (x). The Lie derivative notation is usually preferred whenever higher order derivatives<br />

need to be calculated. Notice that, given two vector fields f, g : D C ]R" -* 1R" we have that<br />

and<br />

and in the special case f = g,<br />

Example 10.1 Let<br />

Then, we have<br />

Lfh(x) = axf(x), Lfh(x) = aX-9(x)<br />

L9Lfh(x) = L9[Lfh(x)] = 2(8xh)g(x)<br />

Lf Lf h(x) = L2 fh(x)<br />

_ 8(Lfh)<br />

1<br />

h(x) = 2 (xi + x2)<br />

8x f (x)<br />

_ _ - 2<br />

XIX2<br />

2<br />

A X ) 9(x) _ -x2 + x Jx2<br />

, .

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