Fully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluids
Implicit constitutive theory provides a very general framework for fluid flow models, including both Newtonian and generalized Newtonian fluids, where the Cauchy stress tensor and the rate of strain tensor are assumed to be related by an implicit relation associated with a maximal monotone graph. Fo...
| Main Authors: | , |
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| Format: | Journal article |
| Language: | English |
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Oxford University Press
2019
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| _version_ | 1797101117361881088 |
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| author | Süli, E Tscherpel, T |
| author_facet | Süli, E Tscherpel, T |
| author_sort | Süli, E |
| collection | OXFORD |
| description | Implicit constitutive theory provides a very general framework for fluid flow models, including both Newtonian and generalized Newtonian fluids, where the Cauchy stress tensor and the rate of strain tensor are assumed to be related by an implicit relation associated with a maximal monotone graph. For incompressible unsteady flows of such fluids, subject to a homogeneous Dirichlet boundary condition on a Lipschitz polytopal domain Ω ⊂ Rd, d ∈ {2, 3}, we investigate a fully discrete approximation scheme, using a spatial mixed finite element approximation on general shape-regular simplicial meshes combined with backward Euler time-stepping. We consider the case when the velocity field belongs to the space of solenoidal functions contained in L∞(0, T; L2(Ω)d) ∩ Lq(0, T; W1,q 0 (Ω)d) with q ∈ (2d/(d + 2),∞), which is the maximal range of q with respect to existence of weak solutions. In order to facilitate passage to the limit with the discretization parameters for the sub-range q ∈ (2d/(d + 2),(3d + 2)/(d + 2)), we introduce a regularization of the momentum equation by means of a penalty term, and first show convergence of a subsequence of approximate solutions to a weak solution of the regularized problem; we then pass to the limit with the regularization parameter. This is achieved by the use of a solenoidal parabolic Lipschitz truncation method, a local Minty-type monotonicity result, and various weak compactness techniques. For q ≥ (3d + 2)/(d + 2) convergence of a subsequence of approximate solutions to a weak solution can be shown directly, without the regularization term. |
| first_indexed | 2024-03-07T05:47:18Z |
| format | Journal article |
| id | oxford-uuid:e7a572cb-8e24-4f34-abcc-9d778354c133 |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-07T05:47:18Z |
| publishDate | 2019 |
| publisher | Oxford University Press |
| record_format | dspace |
| spelling | oxford-uuid:e7a572cb-8e24-4f34-abcc-9d778354c1332022-03-27T10:40:26ZFully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluidsJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:e7a572cb-8e24-4f34-abcc-9d778354c133EnglishSymplectic Elements at OxfordOxford University Press2019Süli, ETscherpel, TImplicit constitutive theory provides a very general framework for fluid flow models, including both Newtonian and generalized Newtonian fluids, where the Cauchy stress tensor and the rate of strain tensor are assumed to be related by an implicit relation associated with a maximal monotone graph. For incompressible unsteady flows of such fluids, subject to a homogeneous Dirichlet boundary condition on a Lipschitz polytopal domain Ω ⊂ Rd, d ∈ {2, 3}, we investigate a fully discrete approximation scheme, using a spatial mixed finite element approximation on general shape-regular simplicial meshes combined with backward Euler time-stepping. We consider the case when the velocity field belongs to the space of solenoidal functions contained in L∞(0, T; L2(Ω)d) ∩ Lq(0, T; W1,q 0 (Ω)d) with q ∈ (2d/(d + 2),∞), which is the maximal range of q with respect to existence of weak solutions. In order to facilitate passage to the limit with the discretization parameters for the sub-range q ∈ (2d/(d + 2),(3d + 2)/(d + 2)), we introduce a regularization of the momentum equation by means of a penalty term, and first show convergence of a subsequence of approximate solutions to a weak solution of the regularized problem; we then pass to the limit with the regularization parameter. This is achieved by the use of a solenoidal parabolic Lipschitz truncation method, a local Minty-type monotonicity result, and various weak compactness techniques. For q ≥ (3d + 2)/(d + 2) convergence of a subsequence of approximate solutions to a weak solution can be shown directly, without the regularization term. |
| spellingShingle | Süli, E Tscherpel, T Fully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluids |
| title | Fully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluids |
| title_full | Fully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluids |
| title_fullStr | Fully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluids |
| title_full_unstemmed | Fully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluids |
| title_short | Fully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluids |
| title_sort | fully discrete finite element approximation of unsteady flows of implicitly constituted incompressible fluids |
| work_keys_str_mv | AT sulie fullydiscretefiniteelementapproximationofunsteadyflowsofimplicitlyconstitutedincompressiblefluids AT tscherpelt fullydiscretefiniteelementapproximationofunsteadyflowsofimplicitlyconstitutedincompressiblefluids |