Slow manifold

In mathematics, the slow manifold of an equilibrium point of a dynamical system occurs as the most common example of a center manifold. One of the main methods of simplifying dynamical systems, is to reduce the dimension of the system to that of the slow manifold—center manifold theory rigorously justifies the modelling.[1][2] For example, some global and regional models of the atmosphere or oceans resolve the so-called quasi-geostrophic flow dynamics on the slow manifold of the atmosphere/oceanic dynamics,[3] and is thus crucial to forecasting with a climate model.

In some cases, a slow manifold is defined to be the invariant manifold on which the dynamics are slow compared to the dynamics off the manifold. The slow manifold in a particular problem would be a sub-manifold of either the stable, unstable, or center manifold, exclusively, that has the same dimension of, and is tangent to, the eigenspace with an associated eigenvalue (or eigenvalue pair) that has the smallest real part in magnitude. This generalizes the definition described in the first paragraph. Furthermore, one might define the slow manifold to be tangent to more than one eigenspace by choosing a cut-off point in an ordering of the real part eigenvalues in magnitude from least to greatest. In practice, one should be careful to see what definition the literature is suggesting.

  1. ^ J. Carr, Applications of centre manifold theory, Applied Math. Sci. 35, 1981, Springer-Verlag
  2. ^ Y. A. Kuznetsov, Elements of applied bifurcation theory, Applied Mathematical Sciences 112, 1995, Springer-Verlag
  3. ^ R. Camassa, On the geometry of an atmospheric slow manifold, Physica D, 84:357–397, 1995.