Finally, we present two numerical examples for finite-time stabilization involving a large-scale dynamical system and a combustion control system.
For an arbitrary H, the function Q ( x ) in formula (1.3) is a distribution which may be (for example, for finite rank H ) very singular.
Finally, we present a numerical example for finite-time stabilization of large-scale impulsive dynamical systems.
(Indeed, for computers and program language, we can only give examples for a finite dimensional space).
Moreover, for finite examples we compare our method to a global analysis, i.e. where in each step the entire state space is considered.
This resulting mesh can serve as direct input for further numerical simulations using, for example, finite element modeling.
Furthermore, many numerical methods for the buckling problem have been studied, for example, finite element schemes [3, 8 12].
As it was shown in the example, this relationship is asymptotic for finite notched bodies and it can be used to calculate a notch stress intensity factor based on a stress concentration results obtained for a notch rounded with small radius of curvature.
For example, finite state machines cannot determine whether an input string consists of some As followed by the same number of Bs.
The latter may be obtained by deterministic modelling of deformations using, for example, finite element method (FEM).
The RBF techniques have more points of interest and have exhibited superior accuracy as compared with traditional numerical strategies, for example, finite difference method (FDM) [20, 23, 47], finite element method (FEM) [23], finite volume method (FVM) [21, 25], and pseudo-spectral method [24].
