22 results on '"Winther, Ragnar"'
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2. The Bubble Transform: A New Tool for Analysis of Finite Element Methods
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Falk, Richard S. and Winther, Ragnar
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Finite element method -- Analysis ,Transformations (Mathematics) -- Analysis ,Mathematics - Abstract
The purpose of this paper is to discuss the construction of a linear operator, referred to as the bubble transform, which maps scalar functions defined on into a collection of functions with local support. In fact, for a given simplicial triangulation of , the associated bubble transform produces a decomposition of functions on [Formula omitted] into a sum of functions with support on the corresponding macroelements. The transform is bounded in both and the Sobolev space , it is local, and it preserves the corresponding continuous piecewise polynomial spaces. As a consequence, this transform is a useful tool for constructing local projection operators into finite element spaces such that the appropriate operator norms are bounded independently of polynomial degree. The transform is basically constructed by two families of operators, local averaging operators and rational trace preserving cutoff operators., Author(s): Richard S. Falk[sup.1] , Ragnar Winther[sup.2] Author Affiliations: (1) Department of Mathematics, Rutgers University, 08854, Piscataway, NJ, USA (2) Department of Mathematics, University of Oslo, 0316, Oslo, Norway Introduction [...]
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- 2016
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3. Smoothed Projections in Finite Element Exterior Calculus
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Christiansen, Snorre H. and Winther, Ragnar
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- 2008
4. Some Superlinear Convergence Results for the Conjugate Gradient Method
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Winther, Ragnar
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- 1980
5. Finite element exterior calculus: from Hodge theory to numerical stability
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Arnold, Douglas N., Falk, Richard S., and Winther, Ragnar
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Finite element method -- Research ,Geometry, Differential -- Research ,Algebraic topology -- Research ,Topology -- Research ,Manifolds (Mathematics) -- Research ,Mathematics - Abstract
This article reports on the confluence of two streams of research, one emanating from the fields of numerical analysis and scientific computation, the other from topology and geometry. In it we consider the numerical discretization of partial differential equations that are related to differential complexes so that de Rham cohomology and Hodge theory are key tools for exploring the well-posedness of the continuous problem. The discretization methods we consider are finite element methods, in which a variational or weak formulation of the PDE problem is approximated by restricting the trial subspace to an appropriately constructed piecewise polynomial subspace. After a brief introduction to finite element methods, we develop an abstract Hilbert space framework for analyzing the stability and convergence of such discretizations. In this framework, the differential complex is represented by a complex of Hilbert spaces, and stability is obtained by transferring Hodge-theoretic structures that ensure well-posedness of the continuous problem from the continuous level to the discrete. We show stable discretization is achieved if the finite element spaces satisfy two hypotheses: they can be arranged into a subcomplex of this Hilbert complex, and there exists a bounded cochain projection from that complex to the subcomplex. In the next part of the paper, we consider the most canonical example of the abstract theory, in which the Hilbert complex is the de Rham complex of a domain in Euclidean space. We use the Koszul complex to construct two families of finite element differential forms, show that these can be arranged in subcomplexes of the de Rham complex in numerous ways, and for each construct a bounded cochain projection. The abstract theory therefore applies to give the stability and convergence of finite element approximations of the Hodge Laplacian. Other applications are considered as well, especially the elasticity complex and its application to the equations of elasticity. Background material is included to make the presentation self-contained for a variety of readers.
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- 2010
6. Stability of a model of human granulopoiesis using continuous maturation
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Astby, Ivar and Winther, Ragnar
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Mathematical models -- Usage ,Differential equations, Partial -- Usage ,Bone cancer -- Models ,Bone cancer -- Research ,Granulocytes -- Research ,Mathematics - Abstract
Byline: Ivar Astby (1), Ragnar Winther (2) Keywords: Stability; Granulopoiesis; Mathematical model Abstract: A class of mathematical models involving a convection-reaction partial differential equation (PDE) is introduced with reference to recovering human granulopoiesis after high dose chemotherapy with stem cell support. The stability properties of the model are addressed by means of numerical investigations and analysis. A simplified model with proliferation rate and mobilization rate independent of maturity shows that the model is stable as the maturation rate grows without bounds, but may go through stable and non-stable regimens as the maturation rate varies. It is also shown that the system is stable when parameters are chosen to approximate a real physiological situation. System characteristics do not change profoundly by introduction of a maturity-dependent proliferation and mobilization rate, as is necessary to make the model operate more in accordance with hematological observations. However, by changing the system mitotic responsiveness with respect to changes in cytokine level, the system is still stable but may show persistent oscillations much resembling clinical observations of cyclic neutropenia. Furthermore, in these cases, changes in the model feedback signal caused by, for instance, an impaired effective cytokine elimination by cell receptors may enforce these oscillations markedly. Author Affiliation: (1) Department of Informatics, University of Oslo, Box 1080, Blindern, 0316, Oslo, Norway (2) Centre of Mathematics for Applications (CMA) and Department of Informatics, 1080, Blindern, 0316, Oslo, Norway Article History: Registration Date: 01/01/2004 Received Date: 24/06/2003 Online Date: 05/07/2004
- Published
- 2004
7. Defferential Complexes and Stability of Finite Element Methods II: The Elasticity Complex.
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Scheel, Arnd, Bochev, Pavel B., Lehoucq, Richard B., Nicolaides, Roy A., Shashkov, Mikhail, Arnold, Douglas N., Falk, Richard S., and Winther, Ragnar
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A close connection between the ordinary de Rham complex and a corresponding elasticity complex is utilized to derive new mixed finite element methods for linear elasticity. For a formulation with weakly imposed symmetry, this approach leads to methods which are simpler than those previously obtained. For example, we construct stable discretizations which use only piecewise linear elements to approximate the stress field and piecewise constant functions to approximate the displacement field. We also discuss how the strongly symmetric methods proposed in [8] can be derived in the present framework. The method of construction works in both two and three space dimensions, but for simplicity the discussion here is limited to the two dimensional case. [ABSTRACT FROM AUTHOR]
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- 2006
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8. Differential Complexes and Stability of Finite Element Methods I. The de Rham Complex.
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Scheel, Arnd, Bochev, Pavel B., Lehoucq, Richard B., Nicolaides, Roy A., Shashkov, Mikhail, Arnold, Douglas N., Falk, Richard S., and Winther, Ragnar
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In this paper we explain the relation between certain piecewise polynomial subcomplexes of the de Rham complex and the stability of mixed finite element methods for elliptic problems. [ABSTRACT FROM AUTHOR]
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- 2006
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9. A uniformly stable Fortin operator for the Taylor-Hood element.
- Author
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Mardal, Kent-Andre, Schöberl, Joachim, and Winther, Ragnar
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CONVEX domains ,TRIANGULATION ,SPEED ,SUBSPACES (Mathematics) ,MATHEMATICS ,SUBSPACE identification (Mathematics) - Abstract
We construct a new Fortin operator for the lowest order Taylor-Hood element, which is uniformly stable both in $$L^2$$ and $$H^1$$. The construction, which is restricted to two space dimensions, is based on a tight connection between a subspace of the Taylor-Hood velocity space and the lowest order Nedelec edge element. General shape regular triangulations are allowed for the $$H^1$$-stability, while some mesh restrictions are imposed to obtain the $$L^2$$-stability. As a consequence of this construction, a uniform inf-sup condition associated the corresponding discretizations of a parameter dependent Stokes problem is obtained, and we are able to verify uniform bounds for a family of preconditioners for such problems, without relying on any extra regularity ensured by convexity of the domain. [ABSTRACT FROM AUTHOR]
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- 2013
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10. Preconditioning discretizations of systems of partial differential equations.
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Mardal, Kent-Andre and Winther, Ragnar
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PARTIAL differential equations , *MATHEMATICS , *LINEAR algebra , *HILBERT space , *METHOD of steepest descent (Numerical analysis) , *ELASTICITY , *CONTROL theory (Engineering) , *SOCIETIES - Abstract
This survey paper is based on three talks given by the second author at the London Mathematical Society Durham Symposium on Computational Linear Algebra for Partial Differential Equations in the summer of 2008. The main focus will be on an abstract approach to the construction of preconditioners for symmetric linear systems in a Hilbert space setting. Typical examples that are covered by this theory are systems of partial differential equations which correspond to saddle point problems. We will argue that the mapping properties of the coefficient operators suggest that block diagonal preconditioners are natural choices for these systems. To illustrate our approach a number of examples will be considered. In particular, parameter-dependent systems arising in areas like incompressible flow, linear elasticity, and optimal control theory will be studied. The paper contains analysis of several models which have previously been discussed in the literature. However, here each example is discussed with reference to a more unified abstract approach. Copyright © 2010 John Wiley & Sons, Ltd. [ABSTRACT FROM AUTHOR]
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- 2011
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11. Applications of the Fourier Transform.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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In this chapter, we briefly discuss the Fourier transform and show how this transformation can be used to solve differential equations where the spatial domain is all of ℝ. [ABSTRACT FROM AUTHOR]
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- 1998
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12. Reaction-Diffusion Equations.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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Reaction-diffusion equations arise as mathematical models in a series of important applications, e.g. in models of superconducting liquids, flame propagation, chemical kinetics, biochemical reactions, predator-prey systems in ecology and so on. Both numerical and mathematical analysis of reaction-diffusion equations are currently very active fields of research. Obviously, we cannot study the subject at an advanced level in the present text, but we can get a general feeling of what these problems are about. Our aim is merely to present some simple models and to explore some of their properties using finite difference schemes and energy estimates. Further examples can be found in the exercises.1 [ABSTRACT FROM AUTHOR]
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- 1998
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13. The Heat Equation Revisited.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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The two previous chapters have been devoted to Fourier series. Of course, the main motivation for the study of Fourier series was their appearance in formal analytic solutions of various partial differential equations like the heat equation, the wave equation, and Poisson's equation. [ABSTRACT FROM AUTHOR]
- Published
- 1998
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14. Convergence of Fourier Series.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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Let f be a piecewise continuous function defined on [-1, 1] with a full Fourier series given by $$ \frac{{a_0 }} {2} + \sum\limits_{k = 1}^\infty {\left( {a_k \cos \left( {k\pi x} \right) + b_k \sin \left( {k\pi x} \right)} \right).} $$ . converge to the function f ?" If we here refer to convergence in the mean square sense, then a partial answer to this question is already established by Theorem 8.2. At least we have seen that we have convergence if and only if the corresponding Parseval's identity holds. However, we like to establish convergence under assumptions which are easier to check. Also, frequently we are interested in notions of convergence other than convergence in the mean. [ABSTRACT FROM AUTHOR]
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- 1998
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15. Orthogonality and General Fourier Series.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
- Abstract
In the previous chapters Fourier series have been the main tool for obtaining formal solutions of partial differential equations. The purpose of the present chapter and the two following chapters is to give a more thorough analysis of Fourier series and formal solutions. The Fourier series we have encountered in earlier chapters can be thought of as examples of a more general class of orthogonal series, and many properties of Fourier series can be derived in this general context. In the present chapter we will study Fourier series from this point of view. The next chapter is devoted to convergence properties of Fourier series, while we return to partial differential equations in Chapter 10. There the goal is to show that the formal solutions are in fact rigorous solutions in a strict mathematical sense. [ABSTRACT FROM AUTHOR]
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- 1998
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16. Poisson's Equation in Two Space Dimensions.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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Poisson's equation is a fundamental partial differential equation which arises in many areas of mathematical physics, for example in fluid flow, flow in porous media, and electrostatics. We have already encountered this equation in Section 6.4 above, where we studied the maximum principle for harmonic functions. As a corollary of the maximum principle we have in fact already established that the Dirichlet problem for Poisson's equation has at most one solution (see Theorem 6.8). [ABSTRACT FROM AUTHOR]
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- 1998
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17. Maximum Principles.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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The purpose of this chapter is to study maximum principles. Such principles state something about the solution of an equation without having to solve it. [ABSTRACT FROM AUTHOR]
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- 1998
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18. Finite Difference Schemes For The Heat Equation.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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In the previous chapter we derived a very powerful analytical method for solving partial differential equations. By using straightforward techniques, we were able find an explicit formula for the solution of many partial differential equations of parabolic type. By studying these analytical solutions, we can learn a lot about the qualitative behavior of such models. This qualitative insight will also be useful in understanding more complicated equations. [ABSTRACT FROM AUTHOR]
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- 1998
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19. The Wave Equation.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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The purpose of this chapter is to study initial-boundary value problems for the wave equation in one space dimension. In particular, we will derive formal solutions by a separation of variables technique, establish uniqueness of the solution by energy arguments, and study properties of finite difference approximations. [ABSTRACT FROM AUTHOR]
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- 1998
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20. The Heat Equation.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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The historical paths of mathematical physics, mathematical analysis, and methods for solving partial differential equations are strongly interlaced, and it is often difficult to draw boundaries between them. In particular, this is the case in the field of Fourier analysis. This field was initiated by Joseph Fourier (1768-1830), a French physicist who studied heat conduction. In his analysis of this problem, he invented the most influential method for solving partial differential equations to this day. For over 200 years his work has been the foundation of certain areas of mathematical analysis. Any student of engineering or of the natural sciences has to master his techniques. [ABSTRACT FROM AUTHOR]
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- 1998
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21. Two-Point Boundary Value Problems.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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In Chapter 1 above we encountered the wave equation in Section 1.4.3 and the heat equation in Section 1.4.4. These equations occur rather frequently in applications, and are therefore often referred to as fundamental equations. We will return to these equations in later chapters. Another fundamental equation is Poisson's equation, given by $$ - \sum\limits_{j = 1}^n {\frac{{\partial ^2 u}} {{\partial x_j^2 }} = f,} $$ where the unknown function u is a function of n spatial variables X1,..., xn. [ABSTRACT FROM AUTHOR]
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- 1998
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22. Setting the Scene.
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Marsden, J. E., Sirovich, L., Golubitsky, M., Jäger, W., Holmes, P., Tveito, Aslak, and Winther, Ragnar
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You are embarking on a journey in a jungle called Partial Differential Equations. Like any other jungle, it is a wonderful place with interesting sights all around, but there are also certain dangerous spots. On your journey, you will need some guidelines and tools, which we will start developing in this introductory chapter. [ABSTRACT FROM AUTHOR]
- Published
- 1998
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