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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.
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Finally, we present a numerical example for finite-time stabilization of large-scale impulsive dynamical systems.
Finally, we present two numerical examples for finite-time stabilization involving a large-scale dynamical system and a combustion control system.
(Indeed, for computers and program language, we can only give examples for a finite dimensional space).
The proposed methodology is illustrated by a realistic numerical example for which the finite element method cannot give correct results.
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].
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].
For example, finite direct sums of Noetherian rings are Noetherian, as is the ring of formal power series over a Noetherian ring.
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