Uniqueness for Weak Solutions to Navier Stokes We proved the following existence result for Navier-Stokes:
|
|
- Buck Dennis
- 5 years ago
- Views:
Transcription
1 Uniqueness for Weak Solutions to Navier Stokes We prove the following existence result for Navier-Stokes: heorem (Existence of a weak solution, n 4) For every f L 0, : V each u 0 H there exists at least one u L 0, : V that is a weak solution of the N-S system In aition, this weak solution satisfies: (a) u L 0, : H u L 4/n 0, : V (b) u t is weakly continuous in H; Uniqueness in the Case n When n, the weak solution has aitional regularity is, in fact, unique heorem (Uniqueness of the weak solution, n ) In the case n, the weak solution of the Navier Stokes equations satisfies: i) u L 0, : V u L 0, : V hence u ~ ũ t C 0, : H ii) u t is unique Proof- We begin by repeating an estimate for the nonlinear term in the N-S system For arbitrary u,v,w H 0 1 U n, we have (by the extene Holer ineqality followe by the C-S inequality) b u,v,w i,j 1 U u i i v j w j x i,j 1 u i 4 i v j w j 4 i,j 1 i v j 1/ i 1 u i 4 1/ j 1 w j 4 1/ In aition, the Sobolev inequality implies where u q C u p u r 1 u C 0 U 0 1, 1/q 1/p 1/n 1 1/r If we choose q 4 p r so that n/4, then with n, we have u 4 C u 1/ u 1/, combine with the previous estimate, 1
2 i 1 u i 4 C i 1 u i u i C u H u V his leas to the following estimate on b u,v,w b u,v,w C u H u V 1/ v V w H w V b u,u,v b u,v,u C u H u V v V u,v V 1/ his implies that B u t V C u H u V Since the weak solution, u t, belongs to L 0, : H L 0, : V, we have 0 B u t V t C 0 u t H t C u u L 0,:V hence B u V C u u L 0,:V B u t L 0, : V hen u t also belongs to L 0, : V then it follows from heorem 3, p87 in Evans that u L 0, : V u L 0, : V implies u t ~ ũ t C 0, : H Now, for u L 0, : V u L 0, : V we have u t,u t V V 1 u t t H hen, if u 1 t, u t are two weak solutions for N-S, let u t u 1 t u t hen u t Au t B u t B u 1 t, u 0 0, u t t H u t V b u t,u t,u t b u 1 t,u 1 t,u t But b u t,u t,u t b u 1 t,u 1 t,u t b u 1 t,u 1 t,u t b u t,u t,u t b u 1 t,u 1 t,u t b u t,u 1 t,u t b u t,u 1 t,u t b u t,u t,u t b u 1 t,u 1 t,u t b u t,u 1 t,u t b u t,u 1 t,u t b u t,u 1 t,u t b u t,u t,u t b u t,u t,u t 0 hen u t t H u t V b u t,u 1 t,u t
3 But as we showe previously, ( using abc C a C b c ) b u t,u 1 t,u t C u t H u 1 t V C C u t V C u t H u 1 t V therefore, u t t H C u t H u 1 t V Since u 1 t V L 1 0,, we get t u t H exp C 0 t u 1 s V s 0 ie, u t H u 0 H 0, or u 1 t u t Summarizing, when n the NS system has a unique solution u t C 0, : H L 0, : V, with u t L 0, : V In aition, u t L 4 U Since the solution is unique in the case n is not unique in the case n 3, it must be that the assumptions uner which a physical flow can be treate as a -imensional flow are also the conitions that preclue turbulence the consequent loss of uniqueness hus a flow which can be treate as -imensional uner some conitions (eg, shallow flow with low flow velocity ) may uner other conitions behave in ways that cannot be viewe as -imensional, even though the flow may still be a shallow flow Uniqueness in the Case n 3 Recall the corollary to the Sobolev inequality implies u 4 C u n/4 u 1 n/4 so that, in the case n 3, we have u 4 C u 3/4 u 1/4 his leas to the result that the weak solution of N-S satisfies, u t L 8/3 0, : L 4 U n, u t L 4/3 0, : V Note that this is strictly weaker than what was true of the solution in the case n 3
4 heorem Suppose n 3 the weak solution of the N-S system satisfies: u t L 0, : H L 0, : V u t L 8 0, : L 4 U n, hen, uner these conitions, u t is unique u t C 0, : H Proof- Supppose u t is a weak solution for N-S with the aitional regularity inicate above hen b u t,u t,v C u t 4 v V u t,v V, implies B u t V C u t 4 0 B u t p V t C 0 u t p 4 t C 0 u t np/ V t It follows that B u t L p 0, : V if u t L 0, : V np/ ; ie, B u t L 4/n 0, : V L 4/3 0, : V On the other h, if u t L 8 0, : L 4 U n, then 0 u t 4 p t for p 4 B u t L 0, : V (at least) hen it follows from the N-S equation that u t L 0, : V this, together with u t L 0, : V imply u t C 0, : H Now observe that b u t,u t,v C 0 u t 4 v 4 C 1 u t 1/4 3/4 v 4 C 1 u t H 1/4 7/4 v 4 Now suppose u 1 t, u t are two weak solutions for N-S both of which have the aitional regularity of the hypotheses Let u t u 1 t u t, note that as in the n proof 4
5 u t t H u t V b u t,u t,u t Also so b u t,u t,u t C 1 u t H 1/4 7/4 u t 4 C u t H u t 4 8 u t t H C u t 8 4 u t H Since u t 4 8 L 1 0,, we can finish the proof as in the n case In the step, u t H 1/4 7/4 u t 4 C u t H u t 4 8 we use the following version of Young s inequality, ab ap p bq q a p C b q, 1 p 1 q 1, a,b 0 5
Tensors, Fields Pt. 1 and the Lie Bracket Pt. 1
Tensors, Fiels Pt. 1 an the Lie Bracket Pt. 1 PHYS 500 - Southern Illinois University September 8, 2016 PHYS 500 - Southern Illinois University Tensors, Fiels Pt. 1 an the Lie Bracket Pt. 1 September 8,
More informationLimiting behaviour of large Frobenius numbers. V.I. Arnold
Limiting behaviour of large Frobenius numbers by J. Bourgain and Ya. G. Sinai 2 Dedicated to V.I. Arnold on the occasion of his 70 th birthday School of Mathematics, Institute for Advanced Study, Princeton,
More informationTHE STOKES SYSTEM R.E. SHOWALTER
THE STOKES SYSTEM R.E. SHOWALTER Contents 1. Stokes System 1 Stokes System 2 2. The Weak Solution of the Stokes System 3 3. The Strong Solution 4 4. The Normal Trace 6 5. The Mixed Problem 7 6. The Navier-Stokes
More informationANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS
ANALYSIS OF A GENERAL FAMILY OF REGULARIZED NAVIER-STOKES AND MHD MODELS MICHAEL HOLST, EVELYN LUNASIN, AND GANTUMUR TSOGTGEREL ABSTRACT. We consier a general family of regularize Navier-Stokes an Magnetohyroynamics
More informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University Sobolev Embedding Theorems Embedding Operators and the Sobolev Embedding Theorem
More information7 Bilinear forms and inner products
7 Bilinear forms and inner products Definition 7.1 A bilinear form θ on a vector space V over a field F is a function θ : V V F such that θ(λu+µv,w) = λθ(u,w)+µθ(v,w) θ(u,λv +µw) = λθ(u,v)+µθ(u,w) for
More informationON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS
ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS Abdelhafid Younsi To cite this version: Abdelhafid Younsi. ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS. 4 pages. 212. HAL Id:
More information2.2 Some Consequences of the Completeness Axiom
60 CHAPTER 2. IMPORTANT PROPERTIES OF R 2.2 Some Consequences of the Completeness Axiom In this section, we use the fact that R is complete to establish some important results. First, we will prove that
More informationAbstract A nonlinear partial differential equation of the following form is considered:
M P E J Mathematical Physics Electronic Journal ISSN 86-6655 Volume 2, 26 Paper 5 Receive: May 3, 25, Revise: Sep, 26, Accepte: Oct 6, 26 Eitor: C.E. Wayne A Nonlinear Heat Equation with Temperature-Depenent
More informationThe effect of dissipation on solutions of the complex KdV equation
Mathematics an Computers in Simulation 69 (25) 589 599 The effect of issipation on solutions of the complex KV equation Jiahong Wu a,, Juan-Ming Yuan a,b a Department of Mathematics, Oklahoma State University,
More informationGLOBAL SOLUTIONS FOR 2D COUPLED BURGERS-COMPLEX-GINZBURG-LANDAU EQUATIONS
Electronic Journal of Differential Equations, Vol. 015 015), No. 99, pp. 1 14. ISSN: 107-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu GLOBAL SOLUTIONS FOR D COUPLED
More informationA COMBUSTION MODEL WITH UNBOUNDED THERMAL CONDUCTIVITY AND REACTANT DIFFUSIVITY IN NON-SMOOTH DOMAINS
Electronic Journal of Differential Equations, Vol. 2929, No. 6, pp. 1 14. ISSN: 172-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu ftp eje.math.txstate.eu A COMBUSTION MODEL WITH UNBOUNDED
More informationPeriodic solutions of a class of nonautonomous second order differential systems with. Daniel Paşca
Periodic solutions of a class of nonautonomous second order differential systems with (q, p) Laplacian Daniel Paşca Abstract Some existence theorems are obtained by the least action principle for periodic
More informationMATH Linear Algebra
MATH 304 - Linear Algebra In the previous note we learned an important algorithm to produce orthogonal sequences of vectors called the Gramm-Schmidt orthogonalization process. Gramm-Schmidt orthogonalization
More informationBLOW-UP AND EXTINCTION OF SOLUTIONS TO A FAST DIFFUSION EQUATION WITH HOMOGENEOUS NEUMANN BOUNDARY CONDITIONS
Electronic Journal of Differential Equations, Vol. 016 (016), No. 36, pp. 1 10. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu BLOW-UP AND EXTINCTION OF SOLUTIONS TO A FAST
More informationarxiv: v1 [math.ap] 17 Feb 2011
arxiv:1102.3614v1 [math.ap] 17 Feb 2011 Existence of Weak Solutions for the Incompressible Euler Equations Emil Wieemann Abstract Using a recent result of C. De Lellis an L. Székelyhii Jr. ( [2]) we show
More informationTheory of PDE Homework 2
Theory of PDE Homework 2 Adrienne Sands April 18, 2017 In the following exercises we assume the coefficients of the various PDE are smooth and satisfy the uniform ellipticity condition. R n is always an
More informationDuality (Continued) min f ( x), X R R. Recall, the general primal problem is. The Lagrangian is a function. defined by
Duality (Continued) Recall, the general primal problem is min f ( x), xx g( x) 0 n m where X R, f : X R, g : XR ( X). he Lagrangian is a function L: XR R m defined by L( xλ, ) f ( x) λ g( x) Duality (Continued)
More informationA generalised Ladyzhenskaya inequality and a coupled parabolic-elliptic problem
A generalised Ladyzhenskaya inequality and a coupled parabolic-elliptic problem Dave McCormick joint work with James Robinson and José Rodrigo Mathematics and Statistics Centre for Doctoral Training University
More informationDiscontinuous Galerkin Methods
Discontinuous Galerkin Methods Joachim Schöberl May 20, 206 Discontinuous Galerkin (DG) methods approximate the solution with piecewise functions (polynomials), which are discontinuous across element interfaces.
More informationResearch Article Brézis-Wainger Inequality on Riemannian Manifolds
Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 2008, Article ID 7596, 6 pages doi:0.55/2008/7596 Research Article Brézis-Wainger Inequality on Riemannian anifolds Przemysław
More informationVariable Exponents Spaces and Their Applications to Fluid Dynamics
Variable Exponents Spaces and Their Applications to Fluid Dynamics Martin Rapp TU Darmstadt November 7, 213 Martin Rapp (TU Darmstadt) Variable Exponent Spaces November 7, 213 1 / 14 Overview 1 Variable
More informationSolution to Homework 8, Math 2568
Solution to Homework 8, Math 568 S 5.4: No. 0. Use property of heorem 5 to test for linear independence in P 3 for the following set of cubic polynomials S = { x 3 x, x x, x, x 3 }. Solution: If we use
More informationChapter 10 Spatial Coherence Part 2
EE90F Chapte0 Spatial Coherence Part Geometry of the fringe pattern: η ( ξ, η ) ξ y Qxy (, ) x ρ ρ r ( ξ, η ) P z pinhole plane viewing plane Define: z + ( x) +( η y) ξ r z + ( x) +( η y) ξ (0.) (0.) ρ
More informationON THE RIEMANN EXTENSION OF THE SCHWARZSCHILD METRICS
ON THE RIEANN EXTENSION OF THE SCHWARZSCHILD ETRICS Valerii Dryuma arxiv:gr-qc/040415v1 30 Apr 004 Institute of athematics an Informatics, AS R, 5 Acaemiei Street, 08 Chisinau, olova, e-mail: valery@ryuma.com;
More informationSupplementary Material of Dynamic Regret of Strongly Adaptive Methods
Supplementary Material of A Proof of Lemma 1 Lijun Zhang 1 ianbao Yang Rong Jin 3 Zhi-Hua Zhou 1 We first prove the first part of Lemma 1 Let k = log K t hen, integer t can be represented in the base-k
More informationhal , version 6-26 Dec 2012
ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS ABDEHAFID YOUNSI Abstract. In this paper, we give a new regularity criterion on the uniqueness results of weak solutions for the 3D Navier-Stokes equations
More informationPDE Notes, Lecture #11
PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =
More informationCOS 511: Theoretical Machine Learning. Lecturer: Rob Schapire Lecture 24 Scribe: Sachin Ravi May 2, 2013
COS 5: heoretical Machine Learning Lecturer: Rob Schapire Lecture 24 Scribe: Sachin Ravi May 2, 203 Review of Zero-Sum Games At the end of last lecture, we discussed a model for two player games (call
More informationHyperbolic Partial Differential Equations
Hyperbolic Partial Differential Equation Evolution equation aociated with irreverible phyical procee like diffuion heat conduction lead to parabolic partial differential equation. When the equation i a
More informationUnderstand the formal definitions of quotient and remainder.
Learning Module 01 Integer Arithmetic and Divisibility 1 1 Objectives. Review the properties of arithmetic operations. Understand the concept of divisibility. Understand the formal definitions of quotient
More informationAn Optimal Algorithm for Bandit and Zero-Order Convex Optimization with Two-Point Feedback
Journal of Machine Learning Research 8 07) - Submitte /6; Publishe 5/7 An Optimal Algorithm for Banit an Zero-Orer Convex Optimization with wo-point Feeback Oha Shamir Department of Computer Science an
More informationTheoretical and numerical results for a chemo-repulsion model with quadratic production
Theoretical and numerical results for a chemo-repulsion model with quadratic production F. Guillén-Gonzalez, M. A. Rodríguez-Bellido & and D. A. Rueda-Gómez Dpto. Ecuaciones Diferenciales y Análisis Numérico
More informationAnisotropic partial regularity criteria for the Navier-Stokes equations
Anisotropic partial regularity criteria for the Navier-Stokes equations Walter Rusin Department of Mathematics Mathflows 205 Porquerolles September 7, 205 The question of regularity of the weak solutions
More informationFunction Spaces. 1 Hilbert Spaces
Function Spaces A function space is a set of functions F that has some structure. Often a nonparametric regression function or classifier is chosen to lie in some function space, where the assume structure
More informationMINIMAL GRAPHS PART I: EXISTENCE OF LIPSCHITZ WEAK SOLUTIONS TO THE DIRICHLET PROBLEM WITH C 2 BOUNDARY DATA
MINIMAL GRAPHS PART I: EXISTENCE OF LIPSCHITZ WEAK SOLUTIONS TO THE DIRICHLET PROBLEM WITH C 2 BOUNDARY DATA SPENCER HUGHES In these notes we prove that for any given smooth function on the boundary of
More informationin Mobile In-App Advertising
Online Appendices to Not Just a Fad: Optimal Sequencing in Mobile In-App Advertising Appendix A: Proofs of echnical Results Proof of heorem : For ease of exposition, we will use a concept of dummy ads
More information1 Convexity explains SVMs
1 Convexity explains SVMs The convex hull of a set is the collection of linear combinations of points in the set where the coefficients are nonnegative and sum to one. Two sets are linearly separable if
More informationLecture I.: (Simple) Basic Variational and Topological Methods (an introductory lecture for graduate students and postdocs)
Lecture I.: (Simple) Basic Variational and Topological Methods (an introductory lecture for graduate students and postdocs) Lecture II.: Regular and Singular Systems with the p- and q-laplacians (an advanced
More informationCOUPLING REQUIREMENTS FOR WELL POSED AND STABLE MULTI-PHYSICS PROBLEMS
VI International Conference on Computational Methos for Couple Problems in Science an Engineering COUPLED PROBLEMS 15 B. Schrefler, E. Oñate an M. Paparakakis(Es) COUPLING REQUIREMENTS FOR WELL POSED AND
More informationLecture 6 Lecturer: Shaddin Dughmi Scribes: Omkar Thakoor & Umang Gupta
CSCI699: opics in Learning & Game heory Lecture 6 Lecturer: Shaddin Dughmi Scribes: Omkar hakoor & Umang Gupta No regret learning in zero-sum games Definition. A 2-player game of complete information is
More informationNONLINEAR FREDHOLM ALTERNATIVE FOR THE p-laplacian UNDER NONHOMOGENEOUS NEUMANN BOUNDARY CONDITION
Electronic Journal of Differential Equations, Vol. 2016 (2016), No. 210, pp. 1 7. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu NONLINEAR FREDHOLM ALTERNATIVE FOR THE p-laplacian
More informationInterconnected Systems of Fliess Operators
Interconnecte Systems of Fliess Operators W. Steven Gray Yaqin Li Department of Electrical an Computer Engineering Ol Dominion University Norfolk, Virginia 23529 USA Abstract Given two analytic nonlinear
More informationResearch Article Global and Blow-Up Solutions for Nonlinear Hyperbolic Equations with Initial-Boundary Conditions
International Differential Equations Volume 24, Article ID 724837, 5 pages http://x.oi.org/.55/24/724837 Research Article Global an Blow-Up Solutions for Nonlinear Hyperbolic Equations with Initial-Bounary
More informationOPTIMAL CONTROL AND STRANGE TERM FOR A STOKES PROBLEM IN PERFORATED DOMAINS
PORTUGALIAE MATHEMATICA Vol. 59 Fasc. 2 2002 Nova Série OPTIMAL CONTROL AND STRANGE TERM FOR A STOKES PROBLEM IN PERFORATED DOMAINS J. Saint Jean Paulin and H. Zoubairi Abstract: We study a problem of
More informationWELL-POSEDNESS OF A POROUS MEDIUM FLOW WITH FRACTIONAL PRESSURE IN SOBOLEV SPACES
Electronic Journal of Differential Equations, Vol. 017 (017), No. 38, pp. 1 7. ISSN: 107-6691. URL: http://eje.math.txstate.eu or http://eje.math.unt.eu WELL-POSEDNESS OF A POROUS MEDIUM FLOW WITH FRACTIONAL
More informationThe Navier-Stokes problem in velocity-pressure formulation :convergence and Optimal Control
The Navier-Stokes problem in velocity-pressure formulation :convergence and Optimal Control A.Younes 1 A. Jarray 2 1 Faculté des Sciences de Tunis, Tunisie. e-mail :younesanis@yahoo.fr 2 Faculté des Sciences
More informationVariational Principles for Equilibrium Physical Systems
Variational Principles for Equilibrium Physical Systems 1. Variational Principles One way of deriving the governing equations for a physical system is the express the relevant conservation statements and
More informationEvolutionary Stability of Pure-Strategy Equilibria in Finite Games
GAMES AND ECONOMIC BEHAVIOR 2, 253265 997 ARTICLE NO GA970533 Evolutionary Stability of Pure-Strategy Equilibria in Finite Games E Somanathan* Emory Uniersity, Department of Economics, Atlanta, Georgia
More informationMULTI-VALUED BOUNDARY VALUE PROBLEMS INVOLVING LERAY-LIONS OPERATORS AND DISCONTINUOUS NONLINEARITIES
MULTI-VALUED BOUNDARY VALUE PROBLEMS INVOLVING LERAY-LIONS OPERATORS,... 1 RENDICONTI DEL CIRCOLO MATEMATICO DI PALERMO Serie II, Tomo L (21), pp.??? MULTI-VALUED BOUNDARY VALUE PROBLEMS INVOLVING LERAY-LIONS
More informationAcute sets in Euclidean spaces
Acute sets in Eucliean spaces Viktor Harangi April, 011 Abstract A finite set H in R is calle an acute set if any angle etermine by three points of H is acute. We examine the maximal carinality α() of
More information2 A Model, Harmonic Map, Problem
ELLIPTIC SYSTEMS JOHN E. HUTCHINSON Department of Mathematics School of Mathematical Sciences, A.N.U. 1 Introduction Elliptic equations model the behaviour of scalar quantities u, such as temperature or
More informationRemarks on Singularities, Dimension and Energy Dissipation for Ideal Hydrodynamics and MHD
Commun. Math. Phys. 184, 443 455 (1997) Communications in Mathematical Physics c Springer-Verlag 1997 Remarks on Singularities, imension an Energy issipation for Ieal Hyroynamics an MH Russel E. Caflisch,
More informationResearch Article On Global Solutions for the Cauchy Problem of a Boussinesq-Type Equation
Abstract and Applied Analysis Volume 202, Article ID 53503, 0 pages doi:0.55/202/53503 esearch Article On Global Solutions for the Cauchy Problem of a Boussinesq-Type Equation Hatice Taskesen, Necat Polat,
More informationANALYSIS CLUB. Restriction Theory. George Kinnear, 7 February 2011
ANALYSIS CLUB Restriction Theory George Kinnear, 7 February 011 The content of this note is base on [Tao10] an [Tao03]. 1 Restriction an extension Our setting is a smooth compact hypersurface S in R (e.g.
More informationThe Generalized Incompressible Navier-Stokes Equations in Besov Spaces
Dynamics of PDE, Vol1, No4, 381-400, 2004 The Generalize Incompressible Navier-Stokes Equations in Besov Spaces Jiahong Wu Communicate by Charles Li, receive July 21, 2004 Abstract This paper is concerne
More informationDesigning Information Devices and Systems II
EECS 16B Fall 2016 Designing Information Devices and Systems II Linear Algebra Notes Introduction In this set of notes, we will derive the linear least squares equation, study the properties symmetric
More informationMath 497 R1 Winter 2018 Navier-Stokes Regularity
Math 497 R Winter 208 Navier-Stokes Regularity Lecture : Sobolev Spaces and Newtonian Potentials Xinwei Yu Jan. 0, 208 Based on..2 of []. Some ne properties of Sobolev spaces, and basics of Newtonian potentials.
More informationMath 360 Linear Algebra Fall Class Notes. a a a a a a. a a a
Math 360 Linear Algebra Fall 2008 9-10-08 Class Notes Matrices As we have already seen, a matrix is a rectangular array of numbers. If a matrix A has m columns and n rows, we say that its dimensions are
More informationSolution of the LLP Limiting case of the Problem of Apollonius via Geometric Algebra, Using Reflections and Rotations
Solution of the LLP Limiting case of the Problem of Apollonius via Geometric Algebra, Using Reflections and Rotations Jim Smith QueLaMateNoTeMate.webs.com email: nitac14b@yahoo.com July 13, 2016 Abstract
More informationMassimo GERMANO Politecnico di Torino
Hybrid Massimo GERMANO Politecnico di Torino Martín SÁNCHEZ-ROCHA Dassault Systèmes SIMULIA Corporation Suresh MENON Georgia Institute of Technology 64th Annual APS-DFD Meeting Baltimore, Maryland November
More informationTHE CORONA FACTORIZATION PROPERTY AND REFINEMENT MONOIDS
THE CORONA FACTORIZATION PROPERTY AND REFINEMENT MONOIDS EDUARD ORTEGA, FRANCESC PERERA, AND MIKAEL RØRDAM ABSTRACT. The Corona Factorization Property of a C -algebra, originally defined to study extensions
More informationarxiv: v1 [math.na] 15 Nov 2017
Noname manuscript No. (will be inserted by the editor) An HDG method with orthogonal projections in facet integrals Issei Oikawa arxiv:1711.05396v1 [math.na] 15 Nov 2017 Received: date / Accepted: date
More informationA PROPERTY OF SOBOLEV SPACES ON COMPLETE RIEMANNIAN MANIFOLDS
Electronic Journal of Differential Equations, Vol. 2005(2005), No.??, pp. 1 10. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) A PROPERTY
More information1. Subspaces A subset M of Hilbert space H is a subspace of it is closed under the operation of forming linear combinations;i.e.,
Abstract Hilbert Space Results We have learned a little about the Hilbert spaces L U and and we have at least defined H 1 U and the scale of Hilbert spaces H p U. Now we are going to develop additional
More informationIntroduction to Turbulence and Turbulence Modeling
Introduction to Turbulence and Turbulence Modeling Part I Venkat Raman The University of Texas at Austin Lecture notes based on the book Turbulent Flows by S. B. Pope Turbulent Flows Turbulent flows Commonly
More informationTHE PRIMITIVE EQUATIONS ON THE LARGE SCALE OCEAN UNDER THE SMALL DEPTH HYPOTHESIS
DISCREE AND CONINUOUS Website: http://aimsciences.org DYNAMICAL SYSEMS Volume 9, Number, January 00 pp. 97 HE PRIMIIVE EQUAIONS ON HE LARGE SCALE OCEAN UNDER HE SMALL DEPH HYPOHESIS Changbing Hu, Roger
More informationFIRST CURVE OF FUČIK SPECTRUM FOR THE p-fractional LAPLACIAN OPERATOR WITH NONLOCAL NORMAL BOUNDARY CONDITIONS
Electronic Journal of Differential Equations, Vol. 208 (208), No. 74, pp. 2. ISSN: 072-669. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu FIRST CURVE OF FUČIK SPECTRUM FOR THE p-fractional
More informationIMA Preprint Series # 2143
A BASIC INEQUALITY FOR THE STOKES OPERATOR RELATED TO THE NAVIER BOUNDARY CONDITION By Luan Thach Hoang IMA Preprint Series # 2143 ( November 2006 ) INSTITUTE FOR MATHEMATICS AND ITS APPLICATIONS UNIVERSITY
More informationA posteriori regularity of the three-dimensional Navier-Stokes equations from numerical computations
A posteriori regularity of the three-dimensional Navier-Stokes equations from numerical computations Sergei I. Chernyshenko, Aeronautics and Astronautics, School of Engineering Sciences, University of
More informationarxiv: v3 [math.ap] 15 Jul 2015
Solving some Navier-Stoes Equations with the initial conditions being some complex-valued periodic functions on R arxiv:1505.0652v [math.ap] 15 Jul 2015 Tao Zhang a, Alatancang Chen a,b,, Fan Bai a a School
More information1. Filling an initially porous tube under a constant head imposed at x =0
Notes on Moving Bounary problems, Voller U o M, volle00@umn.eu. Filling an initially porous tube uner a constant hea impose at x =0 Governing equation is base on calculating the water volume lux by the
More informationSINGULAR PERTURBATION AND STATIONARY SOLUTIONS OF PARABOLIC EQUATIONS IN GAUSS-SOBOLEV SPACES
Communications on Stochastic Analysis Vol. 2, No. 2 (28) 289-36 Serials Publications www.serialspublications.com SINGULAR PERTURBATION AND STATIONARY SOLUTIONS OF PARABOLIC EQUATIONS IN GAUSS-SOBOLEV SPACES
More informationExistence of Positive Solutions to Semilinear Elliptic Systems Involving Concave and Convex Nonlinearities
Journal of Physical Science Application 5 (2015) 71-81 doi: 10.17265/2159-5348/2015.01.011 D DAVID PUBLISHING Existence of Positive Solutions to Semilinear Elliptic Systems Involving Concave Convex Nonlinearities
More informationA posteriori error estimates for non conforming approximation of eigenvalue problems
A posteriori error estimates for non conforming approximation of eigenvalue problems E. Dari a, R. G. Durán b and C. Padra c, a Centro Atómico Bariloche, Comisión Nacional de Energía Atómica and CONICE,
More informationPOINCARÉ S INEQUALITY AND DIFFUSIVE EVOLUTION EQUATIONS
POINCARÉ S INEQUALITY AND DIFFUSIVE EVOLUTION EQUATIONS CLAYTON BJORLAND AND MARIA E. SCHONBEK Abstract. This paper addresses the question of change of decay rate from exponential to algebraic for diffusive
More informationSimplified a priori estimate for the time periodic Burgers equation
Proceedings of the Estonian Academy of Sciences, 21, 59, 1, 34 41 doi: 1.3176/proc.21.1.6 Available online at www.eap.ee/proceedings Simplified a priori estimate for the time periodic Burgers equation
More informationSemidefinite Programming
Semidefinite Programming Notes by Bernd Sturmfels for the lecture on June 26, 208, in the IMPRS Ringvorlesung Introduction to Nonlinear Algebra The transition from linear algebra to nonlinear algebra has
More informationA new regularity criterion for weak solutions to the Navier-Stokes equations
A new regularity criterion for weak solutions to the Navier-Stokes equations Yong Zhou Department of Mathematics, East China Normal University Shanghai 6, CHINA yzhou@math.ecnu.edu.cn Proposed running
More informationThe Dirichlet s P rinciple. In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation:
Oct. 1 The Dirichlet s P rinciple In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation: 1. Dirichlet s Principle. u = in, u = g on. ( 1 ) If we multiply
More informationThe Mollifier Theorem
The Mollifier Theorem Definition of the Mollifier The function Tx Kexp 1 if x 1 2 1 x 0 if x 1, x R n where the constant K is chosen such that R n Txdx 1, is a test function on Rn. Note that Tx vanishes,
More informationMATH 213 Linear Algebra and ODEs Spring 2015 Study Sheet for Midterm Exam. Topics
MATH 213 Linear Algebra and ODEs Spring 2015 Study Sheet for Midterm Exam This study sheet will not be allowed during the test Books and notes will not be allowed during the test Calculators and cell phones
More informationFinite difference MAC scheme for compressible Navier-Stokes equations
Finite difference MAC scheme for compressible Navier-Stokes equations Bangwei She with R. Hošek, H. Mizerova Workshop on Mathematical Fluid Dynamics, Bad Boll May. 07 May. 11, 2018 Compressible barotropic
More informationThe incompressible Navier-Stokes equations in vacuum
The incompressible, Université Paris-Est Créteil Piotr Bogus law Mucha, Warsaw University Journées Jeunes EDPistes 218, Institut Elie Cartan, Université de Lorraine March 23th, 218 Incompressible Navier-Stokes
More informationDiscrete Geometry. Problem 1. Austin Mohr. April 26, 2012
Discrete Geometry Austin Mohr April 26, 2012 Problem 1 Theorem 1 (Linear Programming Duality). Suppose x, y, b, c R n and A R n n, Ax b, x 0, A T y c, and y 0. If x maximizes c T x and y minimizes b T
More informationarxiv: v1 [physics.flu-dyn] 8 May 2014
Energetics of a flui uner the Boussinesq approximation arxiv:1405.1921v1 [physics.flu-yn] 8 May 2014 Kiyoshi Maruyama Department of Earth an Ocean Sciences, National Defense Acaemy, Yokosuka, Kanagawa
More informationOn some parabolic systems arising from a nuclear reactor model
On some parabolic systems arising from a nuclear reactor moel Kosuke Kita Grauate School of Avance Science an Engineering, Wasea University Introuction NR We stuy the following initial-bounary value problem
More informationRelation between Distributional and Leray-Hopf Solutions to the Navier-Stokes Equations
Relation between Distributional and Leray-Hopf Solutions to the Navier-Stokes Equations Giovanni P. Galdi Department of Mechanical Engineering & Materials Science and Department of Mathematics University
More informationEuler Equations: local existence
Euler Equations: local existence Mat 529, Lesson 2. 1 Active scalars formulation We start with a lemma. Lemma 1. Assume that w is a magnetization variable, i.e. t w + u w + ( u) w = 0. If u = Pw then u
More informationExact Internal Controllability for the Semilinear Heat Equation
JOURNAL OF MAEMAICAL ANALYSIS AND APPLICAIONS, 587 997 ARICLE NO AY975459 Exact Internal Controllability for the Semilinear eat Equation Weijiu Liu* and Graham Williams Department of Mathematics, Uniersity
More informationEXISTENCE RESULTS FOR QUASILINEAR HEMIVARIATIONAL INEQUALITIES AT RESONANCE. Leszek Gasiński
DISCRETE AND CONTINUOUS Website: www.aimsciences.org DYNAMICAL SYSTEMS SUPPLEMENT 2007 pp. 409 418 EXISTENCE RESULTS FOR QUASILINEAR HEMIVARIATIONAL INEQUALITIES AT RESONANCE Leszek Gasiński Jagiellonian
More informationLecture Notes: African Institute of Mathematics Senegal, January Topic Title: A short introduction to numerical methods for elliptic PDEs
Lecture Notes: African Institute of Mathematics Senegal, January 26 opic itle: A short introduction to numerical methods for elliptic PDEs Authors and Lecturers: Gerard Awanou (University of Illinois-Chicago)
More informationUNDERGROUND LECTURE NOTES 1: Optimality Conditions for Constrained Optimization Problems
UNDERGROUND LECTURE NOTES 1: Optimality Conditions for Constrained Optimization Problems Robert M. Freund February 2016 c 2016 Massachusetts Institute of Technology. All rights reserved. 1 1 Introduction
More informationA note on the generic solvability of the Navier-Stokes equations
RENDICONTI del SEMINARIO MATEMATICO della UNIVERSITÀ DI PADOVA PAOLO SECCHI A note on the generic solvability of the Navier-Stokes equations Rendiconti del Seminario Matematico della Università di Padova,
More informationA class of domains with fractal boundaries: Functions spaces and numerical methods
A class of domains with fractal boundaries: Functions spaces and numerical methods Yves Achdou joint work with T. Deheuvels and N. Tchou Laboratoire J-L Lions, Université Paris Diderot École Centrale -
More informationSpectral Theorem for Self-adjoint Linear Operators
Notes for the undergraduate lecture by David Adams. (These are the notes I would write if I was teaching a course on this topic. I have included more material than I will cover in the 45 minute lecture;
More informationLecture: Wave-induced Momentum Fluxes: Radiation Stresses
Chapter 4 Lecture: Wave-induced Momentum Fluxes: Radiation Stresses Here we derive the wave-induced depth-integrated momentum fluxes, otherwise known as the radiation stress tensor S. These are the 2nd-order
More informationINVEX FUNCTIONS AND CONSTRAINED LOCAL MINIMA
BULL. AUSRAL. MAH. SOC. VOL. 24 (1981), 357-366. 9C3 INVEX FUNCIONS AND CONSRAINED LOCAL MINIMA B.D. CRAVEN If a certain weakening of convexity holds for the objective and all constraint functions in a
More informationDiscrete Data Assimilation in the Lorenz and 2D Navier Stokes Equations
Discrete Data Assimilation in the Lorenz and 2D Navier Stokes Equations Kevin Hayden 1, Eric Olson 2 and Edriss S. Titi 3,4,5 Consider a continuous dynamical system for which partial information about
More information