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140122 ||| eng |
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|a 9783642870477
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|a Thomasset, F.
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|a Implementation of Finite Element Methods for Navier-Stokes Equations
|h Elektronische Ressource
|c by F. Thomasset
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| 250 |
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|a 1st ed. 1981
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| 260 |
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|a Berlin, Heidelberg
|b Springer Berlin Heidelberg
|c 1981, 1981
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| 300 |
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|a VIII, 164 p. 9 illus
|b online resource
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|a Notations -- 1. Elliptic Equations of Order 2: Some Standard Finite Element Methods -- 1.1. A 1-Dimensional Model Problem: The Basic Notions -- 1.2. A 2-Dimensional Problem -- 1.3. The Finite Element Equations -- 1.4. Standard Examples of Finite Element Methods -- 1.5. Mixed Formulation and Mixed Finite Element Methods for Elliptic Equations -- 2. Upwind Finite Element Schemes -- 2.1. Upwind Finite Differences -- 2.2. Modified Weighted Residual (MWR) -- 2.3. Reduced Integration of the Advection Term -- 2.4. Computation of Directional Derivatives at the Nodes -- 2.5. Discontinuous Finite Elements and Mixed Interpolation -- 2.6. The Method of Characteristics in Finite Elements -- 2.7. Peturbation of the Advective Term: Bredif (1980) -- 2.8. Some Numerical Tests and Further Comments -- 3. Numerical Solution of Stokes Equations -- 3.1. Introduction -- 3.2. Velocity—Pressure Formulations: Discontinuous Approximations of the Pressure -- 3.3. Velocity—Pressure Formulations: Continuous Approximation of the Pressure and Velocity -- 3.4. Vorticity—Pressure—Velocity Formulations: Discontinuous Approximations of Pressure and Velocity -- 3.5. Vorticity Stream-Function Formulation: Decompositions of the Biharmonic Problem -- 4. Navier-Stokes Equations: Accuracy Assessments and Numerical Results -- 4.1. Remarks on the Formulation -- 4.2. A review of the Different Methods -- 4.3. Some Numerical Tests -- 5. Computational Problems and Bookkeeping -- 5.1. Mesh Generation -- 5.2. Solution of the Nonlinear Problems -- 5.3. Iterative and Direct Solvers of Linear Equations -- Appendix 2. Numerical Illustration -- Three Dimensional Case -- References
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| 653 |
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|a Continuum mechanics
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|a Mathematical physics
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|a Continuum Mechanics
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| 653 |
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|a Theoretical, Mathematical and Computational Physics
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| 653 |
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|a Mathematical Methods in Physics
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|a eng
|2 ISO 639-2
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| 989 |
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|b SBA
|a Springer Book Archives -2004
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|a Scientific Computation
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|a 10.1007/978-3-642-87047-7
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|u https://doi.org/10.1007/978-3-642-87047-7?nosfx=y
|x Verlag
|3 Volltext
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|a 531.7
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|a In structure mechanics analysis, finite element methods are now well estab lished and well documented techniques; their advantage lies in a higher flexibility, in particular for: (i) The representation of arbitrary complicated boundaries; (ii) Systematic rules for the developments of stable numerical schemes ap proximating mathematically wellposed problems, with various types of boundary conditions. On the other hand, compared to finite difference methods, this flexibility is paid by: an increased programming complexity; additional storage require ment. The application of finite element methods to fluid mechanics has been lagging behind and is relatively recent for several types of reasons: (i) Historical reasons: the early methods were invented by engineers for the analysis of torsion, flexion deformation of bearns, plates, shells, etc ... (see the historics in Strang and Fix (1972) or Zienckiewicz (1977». (ii) Technical reasons: fluid flow problems present specific difficulties: strong gradients,l of the velocity or temperature for instance, may occur which a finite mesh is unable to properly represent; a remedy lies in the various upwind finite element schemes which recently turned up, and which are reviewed in chapter 2 (yet their effect is just as controversial as in finite differences). Next, waves can propagate (e.g. in ocean dynamics with shallowwaters equations) which will be falsely distorted by a finite non regular mesh, as Kreiss (1979) pointed out. We are concerned in this course with the approximation of incompressible, viscous, Newtonian fluids, i.e. governed by N avier Stokes equations
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