2003
DOI: 10.1002/nme.622
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A LATIN computational strategy for multiphysics problems: application to poroelasticity

Abstract: Multiphysics phenomena and coupled-eld problems usually lead to analyses which are computationally intensive. Strategies to keep the cost of these problems aordable are of special interest. For coupled uid–structure problems, for instance, partitioned procedures and staggered algorithms are often preferred to direct analysis. In this paper, we describe a new strategy for solving coupled multiphysics problems which is built upon the LArge Time INcrement (LATIN) method. The proposed application concerns the cons… Show more

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Cited by 37 publications
(63 citation statements)
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“…Indeed, for such a condition to be taken into account, the descent search direction can no longer be written as (36), but must be expressed in the weak form (37), with a test function F ⋆ which no longer belongs to F, but to F ad instead. The substructure part of (37) remains unchanged:…”
Section: Relation With Newton-schur Domain Decomposition Methodsmentioning
confidence: 99%
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“…Indeed, for such a condition to be taken into account, the descent search direction can no longer be written as (36), but must be expressed in the weak form (37), with a test function F ⋆ which no longer belongs to F, but to F ad instead. The substructure part of (37) remains unchanged:…”
Section: Relation With Newton-schur Domain Decomposition Methodsmentioning
confidence: 99%
“…This technique, which is commonly used in the LATIN method [19], consists in defining an approximation based on generalized radial functions. It has been shown in previous works [19,37,29] that under small-displacement assumptions this approach reduces the computational cost drastically. All the details can be found in [16].…”
Section: Radial Loading Approximationmentioning
confidence: 99%
“…; u F ðx; tÞ defined in a space-time domain X Â I. These fields can be related to different physics (various examples can be found in [19,32,33,6,10]) or as illustrated in [9,18], they can be different components of a vector field. Also, we allow different approximation spaces for each field, that is the discrete representation of a given field u i is stored in a second order tensor u i 2 R Nði;SÞ R Nði;TÞ (where Nði; dÞ gives the size of the approximation space related to the field i in the dimension d ¼ S or T).…”
Section: Extension To Multi-field Modelsmentioning
confidence: 99%
“…Following approaches used in [19,32,6,9,18,10], we introduce a rank-M approximation 3 of each second order tensor u i . We denote this multi-field decomposition fug M and define the corresponding subset S…”
Section: Optimal Approximation With Respect To the Target Normmentioning
confidence: 99%
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