Abstract
Without the assumption that the coefficient of weak damping is large enough, the existence of the global random attractors for simplified Von Karman plate without rotational inertia driven by either additive white noise or multiplicative white noise are proved. Instead of the classical splitting method, the techniques to verify the asymptotic compactness rely on stabilization estimation of the system. Furthermore, a clear relationship between in-plane components of the external force that act on the edge of the plate and the expectation of radius of the global random attractors can be obtained from the theoretical results. Based on the relationship between global random attractor and random probability invariant measure, the global dynamics of the plates are analyzed numerically. With increasing the in-plane components of the external force that act on the edge of the plate, global D-bifurcation, secondary global D-bifurcation and complex local dynamical behavior occur in motion of the system. Moreover, increasing the intensity of white noise leads to the dynamical behavior becoming simple. The results on global dynamics reveal that random snap-through which seems to be a complex dynamics intuitively is essentially a simple dynamical behavior.
Highlights
There exists an essential difference between full Von Karman plate without rotational inertia and simplified Von Karman plate without rotational inertia
The definition of global random attractors for random dynamical system (RDS) established by Arnold [4] were proposed by Crauel and Flandoli [5] and Schmalfuss [6]
The purpose of this paper is to investigate the existence of global random attractors for SAVKP and SMVKP and to derive the global dynamics by achieving the structure of their global random attractors
Summary
The governing equations of full Von Karman plates without rotational inertia comprise coupled plate equations and wave equations, while the coupled plate equation and elliptic equation compose the governing equations of Von Karman plate [3]. The definition of global random attractors for random dynamical system (RDS) established by Arnold [4] were proposed by Crauel and Flandoli [5] and Schmalfuss [6]. The former developed the theory of global random attractors in phase space, while the random attractor is seen as a subset in the space of probability measures by Schmalfuss. The assertion that global random attractors are uniquely determined by Symmetry 2018, 10, 315; doi:10.3390/sym10080315 www.mdpi.com/journal/symmetry
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