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Hyperbolic Fixed Points: . Saddles, Sources, and Sinks

 

Let tex2html_wrap_inline15145 be an equilibrium point of a vector field. Then tex2html_wrap_inline15098 is called a hyperbolic  fixed point if none of the real parts of the eigenvalues of tex2html_wrap_inline15124 is equal to zero. The test for asymptotic stability of the previous section can be restated as: a hyperbolic fixed point is stable if the real parts of all its eigenvalues are negative. A fixed point of a map is hyperbolic if none of the moduli of the eigenvalues equals one.

The motion near a hyperbolic fixed point can be analyzed and brought into a standard form by a linear transformation to the eigenvectors of tex2html_wrap_inline15124 . Additional analysis, including higher-order terms, is usually needed to analyze the motion near a nonhyperbolic fixed point.

At last, we can precisely define the terms saddle, sink, source, and center. A hyperbolic equilibrium solution is a saddle  if the real part of at least one eigenvalue of the linearized vector field is less than zero and if the real part of at least one eigenvalue is greater than zero. Similarly, a saddle point for a map is a hyperbolic point if at least one of the eigenvalues of the associated linear map has a modulus greater than one, and if one of the eigenvalues has modulus less than one.

A hyperbolic point of a flow is a stable node  or sink  if all the eigenvalues have real parts less than zero. Similarly, if all the moduli are less than one then the hyperbolic point of a map is a sink.

A hyperbolic point is an unstable node  or source  if the real parts of all the eigenvalues are greater than zero. The moduli of a source of a map are all greater than one.

A center  is a nonhyperbolic fixed point for which all the eigenvalues are purely imaginary and nonzero (modulus one for maps). For a picture of the elementary equilibrium points in three-dimensional space see Figure 3.10 of Thompson and Stewart [7]. The corresponding stability information for a hyperbolic fixed point of a two-dimensional map is summarized in Figure 4.9.

   figure4947
Figure 4.9: Complex eigenvalues for a two-dimensional map with a hyperbolic fixed point: (a) saddle, (b) sink, and (c) source.


next up previous contents
Next: Invariant Manifolds Up: Fixed Points Previous: Linearization

Nicholas B. Tufillaro
Mon Mar 3 01:58:02 PST 1997