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A nonparametric stochastic model for non-Gaussian random fields with SO(n,R)-invariance

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HAL Id: hal-00734171

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Submitted on 20 Sep 2012

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A nonparametric stochastic model for non-Gaussian random fields with SO(n,R)-invariance

Johann Guilleminot, Christian Soize

To cite this version:

Johann Guilleminot, Christian Soize. A nonparametric stochastic model for non-Gaussian random fields with SO(n,R)-invariance. Congress on Computational Methods in Applied Sciences and En- gineering (ECCOMAS 2012), Vienna University of Technology, Sep 2012, Vienna, Austria. pp.1-2.

�hal-00734171�

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A nonparametric stochastic model for non-Gaussian random fields with SO(n,R)-invariance

J. Guilleminot†∗, C. Soize

Universit´e Paris-Est

Laboratoire Mod´elisation et Simulation Multi Echelle, MSME UMR 8208 CNRS 5 Bd Descartes, 77454 Marne la Vall´ee, France

johann.guilleminot@univ-paris-est.fr christian.soize@univ-paris-est.fr

Keywords: random fields, invariance, MaxEnt, non-Gaussian, probabilistic model.

ABSTRACT

In this work, we address the construction of a generalized nonparametric probabilistic model for matrix- valued non-Gaussian random fields exhibiting some invariance properties with respect to given ortho- gonal transformations. Such an issue naturally arises in linear elasticity, where the so-called material symmetries are defined in terms of someSO(n,R)-invariance. Hereinafter, we denote asx7→ [C(x)]

the elasticity tensor random field, the probability model of which must be constructed. It is defined on a given probability space, indexed by a bounded domainRdand takes its values in a given subset Msymn (R)of the setM+n(R)of all the positive-definite symmetric(n×n)real matrices. First, we present a probabilistic model, the construction of which relies on the overall methodology introduced in [2]

and which extends the results derived in [4] for random elasticity matrices. Specifically, the approach introduces a particular algebraic form for the random fieldx 7→ [C(x)]and involves two additional random fieldsx 7→ [S(x)]andx 7→ [A(x)], indexed byand taking their values in Msymn (R) and M+n(R)respectively, such that

[C(x)] = [S(x)] [A(x)] [S(x)] (1)

for allxinΩ. The representation is therefore based on two independent sources of uncertainties, one preserving almost surely the topological structure inMsymn (R)(namely, the random fieldx7→ [S(x)]) and the other one acting as an anisotropic stochastic germ. The family of first-order marginal probability distributions is prescribed through a nonlinear mapping acting on a set of normalized Gaussian random fields, the definition of which is obtained by having recourse to the maximum entropy principle [1]. In practice, such a representation allows the level of statistical fluctuations of the random field to be uncou- pled from the level of fluctuations associated with a stochastic measure of anisotropy. Next we propose a novel numerical strategy for the random generation of the random field. The algorithm consists in solving a family of Itˆo stochastic differential equations (see [3]) and turns out to be very efficient as the stochastic dimension increases. It is worth noting that unlike the alternative polynomial-chaos based strategy, which typically involves identification procedures (for the coefficients) based on matching the first-order marginal distributions, the algorithm allows for the preservation of the statistical dependence - between the components of the simulated random variables - at no additional computational cost. A new discretization scheme is also proposed. Finally, the approach and algorithms are exemplified by considering the classes of isotropic and transversely isotropic tensors. For instance, the graphs of the first-order marginal probability density functions of componentsC11andC12at an arbitrary point are displayed below and shows the nongaussianity of the modeled random field.

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6 8 10 12 14 16 10−7

10−6 10−5 10−4 10−3 10−2 10−1 100

c pC11(c)

−4 −2 0 2 4 6

10−7 10−6 10−5 10−4 10−3 10−2 10−1 100

c p C12(c)

Figure 1: Graph of the probability density functionc7→pC11(c)(left) andc7→pC12(c)(right).

References

[1] E.T. Jaynes: Information theory and statistical mechanics. Phys. Rev., 106/108 (1957), 620–

630/171–190.

[2] C. Soize: Non-Gaussian positive-definite matrix-valued random fields for elliptic stochastic partial differential operators.Computer methods in applied mechanics and engineering, 195 (2006), 26–

64.

[3] C. Soize: Construction of probability distributions in high dimension using the maximum entropy principle: Applications to stochastic processes, random fields and random matrices.International Journal for Numerical Methods in Engineering, 76 (2008), 1583–1611.

[4] J. Guilleminot, C. Soize: Generalized Stochastic Approach for Constitutive Equation in Linear Elasticity: A Random Matrix Model.International Journal for Numerical Methods in Engineer- ing, (2011), accepted for publication on September 18 2011.

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