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84 CHAPTER 3. LYAPUNOV STABILITY I. AUTONOMOUS SYSTEMS<br />

Proof: See the Appendix.<br />

We now put these ideas to work using the following example.<br />

Example 3.10 Consider the following system:<br />

.i1 = -axl<br />

2 = bx2 + xlx2.<br />

Clearly, the origin is an equilibrium point. To study the stability of this equilibrium point,<br />

we proceed to find a Lyapunov function as follows.<br />

Step 1: Assume that VV(x) = g(x) has the form<br />

Step 2: Impose the symmetry conditions,<br />

In our case we have<br />

02V<br />

x1 + h2x2]. (3.8)<br />

g(x) = [hlxl + hix2, hl2 2<br />

2<br />

as,, - ag,<br />

= a V or, equivalently<br />

axtax, ax, ax, ax; - ax,<br />

1991<br />

ahl<br />

xl ahl + h2 + x2<br />

ax2 ax2 ax2<br />

19x1<br />

= h2 + x1<br />

1 2<br />

ax,<br />

+ x2 axl .<br />

To simplify the solution, we attempt to solve the problem assuming that the J, 's are constant.<br />

If this is the case, then<br />

ahi = ahi = ah2 = ah2 = 0<br />

ax2 ax2 19x1 axl<br />

and we have that:<br />

In particular, choosing k = 0, we have<br />

1991 1992 = hl 2 =1 h2 = k<br />

ax2 19x1<br />

g(x) = [hlxl + kx2i kxl + h2x2].<br />

9(x) = [91, 92] = [hlxl, h2x2]

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