2015
DOI: 10.1016/j.camwa.2015.02.012
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Stochastic exponential integrator for finite element spatial discretization of stochastic elastic equation

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Cited by 4 publications
(2 citation statements)
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“…The deterministic counterpart of (1.1) finds many applications in viscoelastic theory [7,15,16], and its linear version has been numerically studied by [14,21], where a finite element method is used for spatial discretization and rational approximations for analytic semigroup. Particularly when α = 0, the problem (1.1) reduces to a stochastic wave equation (SWE) without damping, numerical approximations of which have been recently studied by many authors [2][3][4][5][8][9][10][11][12][17][18][19][22][23][24]. In contrast to the SWE case (α = 0), the stochastic strongly damped wave equations (α > 0) are much less well-understood, from both theoretical and numerical point of view.…”
Section: Introductionmentioning
confidence: 99%
“…The deterministic counterpart of (1.1) finds many applications in viscoelastic theory [7,15,16], and its linear version has been numerically studied by [14,21], where a finite element method is used for spatial discretization and rational approximations for analytic semigroup. Particularly when α = 0, the problem (1.1) reduces to a stochastic wave equation (SWE) without damping, numerical approximations of which have been recently studied by many authors [2][3][4][5][8][9][10][11][12][17][18][19][22][23][24]. In contrast to the SWE case (α = 0), the stochastic strongly damped wave equations (α > 0) are much less well-understood, from both theoretical and numerical point of view.…”
Section: Introductionmentioning
confidence: 99%
“…Great attention has been devoted in the last decades to numerical approximations of evolutionary stochastic partial differential equations (SPDEs) (see, e.g. [2,4,9,11,12,21,23,25] and references therein). In the present work, we concentrate on a class of semi-linear SPDEs of second order with damping, described by    du t = αLu t dt + Lu dt + F (u) dt + dW (t), in D × (0, T ], u(·, 0) = u 0 , u t (·, 0) = v 0 , in D, u = 0, on ∂D × (0, T ], The initial data u 0 , v 0 are assumed to be F 0 -measurable random variables.…”
Section: Introductionmentioning
confidence: 99%