In dynamical systems theory, the Olech theorem establishes sufficient conditions for global asymptotic stability of a two-equation system of non-linear differential equations. The result was established by Czesław Olech in 1963,[1] based on joint work with Philip Hartman.[2]
The differential equations
|
=f(x)
x=[x1
T | |
x | |
2] |
\inR2
f(x)=\begin{bmatrix}f1(x)&f2(x)\end{bmatrix}T
x\ast=0
(a) the trace of the Jacobian matrix is negative,
\operatorname{tr}Jf(x)<0
x\inR2
(b) the Jacobian determinant is positive,
\left|Jf(x)\right|>0
x\inR2
(c) the system is coupled everywhere with either
\partialf1 | |
\partialx1 |
\partialf2 | |
\partialx2 |
≠ 0, or
\partialf1 | |
\partialx2 |
\partialf2 | |
\partialx1 |
≠ 0forallx\inR2.