Math 497 R1 Winter 2018 Navier-Stokes Regularity

Size: px
Start display at page:

Download "Math 497 R1 Winter 2018 Navier-Stokes Regularity"

Transcription

1 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. Table of contents. Sobolev Spaces Lebesgue spaces Sobolev spaces Newtonian Potentials Bibliography

2 2 Navier-Stokes Regularity.. Lebesgue spaces. Sobolev Spaces Lemma. (Lemma. of []) Let 6 p <, then L p () is the completion of C 0 () in L p (). Proof.. We have = [B n where B n has center x n 2 rational and radius r n = 2 dist(x n; c ). 2. We also have can be approximated from within by compact sets C m such that the measure of the dierence C m goes to zero. 3. Each C m can be covered by nitely many B n 's. Denote the union of these balls by m. We now have dist ( m ; c ) > 0 and kuk Lp ( m )! Now mollify u m to get u m 2 C 0 (). Remark 2. i. Note that is only required to be a domain (open connected set). No regularity is needed ii. It is obvious that L is not the completion of C 0. Question 3. What about Lorentz spaces?.2. Sobolev spaces Definition 4. (Sobolev spaces) W k s (). L s integrability of weak derivatives. k kuk Ws k () = X i=0 kr i uk s; : () W s k (). W k s completion of C 0 (). L k s (). L s integrability of r k u. kuk Ls k () = krk uk s; : (2) L s k (). L s k completion of C 0 () in the following sense. [u] 2 L s k () is an equivalence class of functions satisfying a) 8v; w 2 [u], r k (v w) = 0, and b) 9u 0 2 [u] such that there exists u m 2 C 0 () with kr k (u m u 0 )k s;! 0. It turns out that integrability of derivative implies local integrability of the function. Theorem 5. (Theorem.) u 2 L s k () =) u 2 L s;loc (). Proof. It suces to prove for k =. Once this is done, the general case follows easily from induction. By assumption, for any ' 2 C 0 () we have hu; r'i = R g ' for some g 2 L s(). We need to prove, for any 0 b, u 2 L s ( 0 ). The main diculty lies in construction of the function u which is well-dened in the whole.

3 X Yu 3 Now x one such 0. Let 0 < " < dist( 0 ; c ). Let u " be the standard mollication of the distribution u. i. We rst show that u " 2 L ( 0 ) for each ". To see this, dene l: L ( 0 ) 7! R by l( ) := hu; " i: (3) As u 2 D 0 (), there is m 2 N [ f0g such that jl( )j 6 C k " k C m () 6 C(") k k L ( 0 ). Thus by Riesz representation theorem we have u " 2 L ( 0 ). ii. Now we easily see that g " = ru " in 0. iii. Next let u 0;" := u " [u " ] 0 where [u " ] 0 is the average of u " in 0. By Poincare's inequality we have u 0;"! u 0 in L s ( 0 ).??? Naturally g = ru 0 in 0. iv. Now we need to construct u, dened on, such that uj 0 =u 0. Let c 0 and b. Repeating the above we have u 2 L s ( ) such that g = ru in. As r(u u 0 ) = 0 in 0, u u 0 = C 0, a constant, in 0. We re-dene u C 0 2 L s ( ) as the new u. This can be repeated for a nested sequence of sets 0 b b 2 b b. Note that in each m, we have u m = u m+ = u m+2 =. Thus convergence is not an issue. Finally, any other v with rv = g is just a constant away from the u just constructed. Remark 6. It is clear that we cannot expect u 2 L s (). For example let = R and s =, and u = jxj. Corollary 7. If u m 2 C 0 () is Cauchy in L s k, then there is u 2 L s k () such that ku m uk Ls k ()! 0. Remark 8. The proof is similar to that of Theorem 5. Also note that does not need to be bounded here. Corollary 9. (Proposition.2) For bounded domain, L s k () = W s k (). Proof. Clearly W s k () L s k (). For the other direction, we need to show that for every [u] 2 L s k (), there must exist a v 2 [u] such that v 2 W s k (). Let [u] 2 L s k (). By denition there is w 2 L s;loc () such that i. For every other w 0 2 [u], r k (w w 0 ) = 0; ii. There is a sequence w m 2 C 0 () such that r k w m! r k w in L s (). As is bounded, we have Friedrichs inequality: kw m w m 0k Ls () 6 c kr k w m r k w m 0k Ls () (4) which can be obtained through repeated application of Poincaré. Thus w m converges in L s, to some function v. It is clear that v 2 [u]. Remark 0. When n > 3, thanks to the Gagliardo-Nirenberg inequality kuk p; 6 c(n) kruk 2; where p = 2 n n 2, we see that L 2 () L p (), in the sense that for every [u] 2 L 2 (), there is a w 2 [u] such that w 2 L p. When n = 2 and = R + 2, we can still select a good representative for every [u] 2 L 2 (R + 2 ) by the criterion kvk L2 () < where = R (0; ). =)Any with good boundary would be OK?. is bounded.

4 4 Navier-Stokes Regularity 2. Newtonian Potentials Recall the fundamental solutions 8 >< E(x) = >: 2 ln jxj! n n (n 2) We can dene the Newtonian potential of a function f: n = 2 : (5) jxj n 2 n > 3 u = E f: (6) Proposition. (Proposition 2.3) Let f 2 L p (R n ) with < p < and u =E f. Then 4u = f in R n, and u 2 L p 2 (R n ). Furthermore R R n jr 2 uj p dx 6 c(n; p) R R n jf j p dx. Proof. Note that R R n jr 2 uj p dx 6 c(n; p) R R n jf j p dx follows from the theory of singular integral operators. Next notice that for f 2 C 0, 4u = f holds by direct calculation. The general situation now follows from the above estimate and approximation argument. Thus all we need to prove is the existence of u m 2 C 0 such that kr 2 (u m u)k L2 (R n )! 0. Let f m 2 C 0 (R n ), f m! f in L p (R n ). Dene v m = E f m. As f m has compact support, we have jr i v m j 6 c(m; i) jxj n 2+i; x 2 Rn : (7) Now consider R > 0 and let ' R be the standard cut-o function. We calculate Z " Z jr 2 (' R v m v m )j p dx 6 c R n Z 6 c B R c B R c jr 2 v m j p + R p Z B 2R nb R jrv m j p + R 2p Z B 2R nb R jr 2 v m j p jr 2 v m j p + C(m) R n( p) : (8) # Thus for each m, we take R m such that R R n nishes the proof. jr 2 (' Rm v m v m )j p dx < m. Dening u m = ' Rm v m

5 X Yu 5 Bibliography [] Gregory Seregin. Lecture Notes on Regularity Theory for the Navier-Stokes Equations. World Scientic, 205.

ON TRIVIAL GRADIENT YOUNG MEASURES BAISHENG YAN Abstract. We give a condition on a closed set K of real nm matrices which ensures that any W 1 p -grad

ON TRIVIAL GRADIENT YOUNG MEASURES BAISHENG YAN Abstract. We give a condition on a closed set K of real nm matrices which ensures that any W 1 p -grad ON TRIVIAL GRAIENT YOUNG MEASURES BAISHENG YAN Abstract. We give a condition on a closed set K of real nm matrices which ensures that any W 1 p -gradient Young measure supported on K must be trivial the

More information

Introduction to Real Analysis

Introduction to Real Analysis Introduction to Real Analysis Joshua Wilde, revised by Isabel Tecu, Takeshi Suzuki and María José Boccardi August 13, 2013 1 Sets Sets are the basic objects of mathematics. In fact, they are so basic that

More information

Near convexity, metric convexity, and convexity

Near convexity, metric convexity, and convexity Near convexity, metric convexity, and convexity Fred Richman Florida Atlantic University Boca Raton, FL 33431 28 February 2005 Abstract It is shown that a subset of a uniformly convex normed space is nearly

More information

XIAOFENG REN. equation by minimizing the corresponding functional near some approximate

XIAOFENG REN. equation by minimizing the corresponding functional near some approximate MULTI-LAYER LOCAL MINIMUM SOLUTIONS OF THE BISTABLE EQUATION IN AN INFINITE TUBE XIAOFENG REN Abstract. We construct local minimum solutions of the semilinear bistable equation by minimizing the corresponding

More information

2 BAISHENG YAN When L =,it is easily seen that the set K = coincides with the set of conformal matrices, that is, K = = fr j 0 R 2 SO(n)g: Weakly L-qu

2 BAISHENG YAN When L =,it is easily seen that the set K = coincides with the set of conformal matrices, that is, K = = fr j 0 R 2 SO(n)g: Weakly L-qu RELAXATION AND ATTAINMENT RESULTS FOR AN INTEGRAL FUNCTIONAL WITH UNBOUNDED ENERGY-WELL BAISHENG YAN Abstract. Consider functional I(u) = R jjdujn ; L det Duj dx whose energy-well consists of matrices

More information

Rearrangements and polar factorisation of countably degenerate functions G.R. Burton, School of Mathematical Sciences, University of Bath, Claverton D

Rearrangements and polar factorisation of countably degenerate functions G.R. Burton, School of Mathematical Sciences, University of Bath, Claverton D Rearrangements and polar factorisation of countably degenerate functions G.R. Burton, School of Mathematical Sciences, University of Bath, Claverton Down, Bath BA2 7AY, U.K. R.J. Douglas, Isaac Newton

More information

Anisotropic partial regularity criteria for the Navier-Stokes equations

Anisotropic 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 information

Max-Planck-Institut fur Mathematik in den Naturwissenschaften Leipzig A generalization of Rellich's theorem and regularity of varifolds minimizing curvature by Roger Moser Preprint no.: 72 2001 A generalization

More information

Notes on Integrable Functions and the Riesz Representation Theorem Math 8445, Winter 06, Professor J. Segert. f(x) = f + (x) + f (x).

Notes on Integrable Functions and the Riesz Representation Theorem Math 8445, Winter 06, Professor J. Segert. f(x) = f + (x) + f (x). References: Notes on Integrable Functions and the Riesz Representation Theorem Math 8445, Winter 06, Professor J. Segert Evans, Partial Differential Equations, Appendix 3 Reed and Simon, Functional Analysis,

More information

The Erwin Schrodinger International Boltzmanngasse 9. Institute for Mathematical Physics A-1090 Wien, Austria

The Erwin Schrodinger International Boltzmanngasse 9. Institute for Mathematical Physics A-1090 Wien, Austria ESI The Erwin Schrodinger International Boltzmanngasse 9 Institute for Mathematical Physics A-19 Wien, Austria The Negative Discrete Spectrum of a Class of Two{Dimentional Schrodinger Operators with Magnetic

More information

Real Analysis Notes. Thomas Goller

Real Analysis Notes. Thomas Goller Real Analysis Notes Thomas Goller September 4, 2011 Contents 1 Abstract Measure Spaces 2 1.1 Basic Definitions........................... 2 1.2 Measurable Functions........................ 2 1.3 Integration..............................

More information

MARIA GIRARDI Fact 1.1. For a bounded linear operator T from L 1 into X, the following statements are equivalent. (1) T is Dunford-Pettis. () T maps w

MARIA GIRARDI Fact 1.1. For a bounded linear operator T from L 1 into X, the following statements are equivalent. (1) T is Dunford-Pettis. () T maps w DENTABILITY, TREES, AND DUNFORD-PETTIS OPERATORS ON L 1 Maria Girardi University of Illinois at Urbana-Champaign Pacic J. Math. 148 (1991) 59{79 Abstract. If all bounded linear operators from L1 into a

More information

Convergence of A Galerkin Method for 2-D Discontinuous Euler Flows Jian-Guo Liu 1 Institute for Physical Science andtechnology and Department of Mathe

Convergence of A Galerkin Method for 2-D Discontinuous Euler Flows Jian-Guo Liu 1 Institute for Physical Science andtechnology and Department of Mathe Convergence of A Galerkin Method for 2-D Discontinuous Euler Flows Jian-Guo Liu 1 Institute for Physical Science andtechnology and Department of Mathematics University of Maryland College Park, MD 2742

More information

Chapter 3: Baire category and open mapping theorems

Chapter 3: Baire category and open mapping theorems MA3421 2016 17 Chapter 3: Baire category and open mapping theorems A number of the major results rely on completeness via the Baire category theorem. 3.1 The Baire category theorem 3.1.1 Definition. A

More information

system of PenroseFife type Olaf Klein Weierstrass Institute for Applied Analysis and Stochastics Mohrenstrasse 39 D10117 Berlin Germany

system of PenroseFife type Olaf Klein Weierstrass Institute for Applied Analysis and Stochastics Mohrenstrasse 39 D10117 Berlin Germany A class of time discrete schemes for a phaseeld system of PenroseFife type Olaf Klein Weierstrass Institute for Applied Analysis and Stochastics Mohrenstrasse 39 D7 Berlin Germany email: klein@wias-berlin.de

More information

Introduction to Geometric Measure Theory

Introduction to Geometric Measure Theory Introduction to Geometric easure Theory Leon Simon 1 Leon Simon 2014 1 The research described here was partially supported by NSF grants DS-9504456 & DS 9207704 at Stanford University Contents 1 Preliminary

More information

Pointwise convergence rate for nonlinear conservation. Eitan Tadmor and Tao Tang

Pointwise convergence rate for nonlinear conservation. Eitan Tadmor and Tao Tang Pointwise convergence rate for nonlinear conservation laws Eitan Tadmor and Tao Tang Abstract. We introduce a new method to obtain pointwise error estimates for vanishing viscosity and nite dierence approximations

More information

Max-Planck-Institut fur Mathematik in den Naturwissenschaften Leipzig Uniformly distributed measures in Euclidean spaces by Bernd Kirchheim and David Preiss Preprint-Nr.: 37 1998 Uniformly Distributed

More information

N-BLACK HOLE STATIONARY AND AXIALLY EQUATIONS GILBERT WEINSTEIN. Abstract. The Einstein/Maxwell equations reduce in the stationary

N-BLACK HOLE STATIONARY AND AXIALLY EQUATIONS GILBERT WEINSTEIN. Abstract. The Einstein/Maxwell equations reduce in the stationary N-LACK HOLE STATIONARY AND AXIALLY SYMMETRIC SOLUTIONS OF THE EINSTEIN/MAXWELL EQUATIONS GILERT WEINSTEIN Abstract. The Einstein/Maxwell equations reduce in the stationary and axially symmetric case to

More information

THE L 2 -HODGE THEORY AND REPRESENTATION ON R n

THE L 2 -HODGE THEORY AND REPRESENTATION ON R n THE L 2 -HODGE THEORY AND REPRESENTATION ON R n BAISHENG YAN Abstract. We present an elementary L 2 -Hodge theory on whole R n based on the minimization principle of the calculus of variations and some

More information

(1.) For any subset P S we denote by L(P ) the abelian group of integral relations between elements of P, i.e. L(P ) := ker Z P! span Z P S S : For ea

(1.) For any subset P S we denote by L(P ) the abelian group of integral relations between elements of P, i.e. L(P ) := ker Z P! span Z P S S : For ea Torsion of dierentials on toric varieties Klaus Altmann Institut fur reine Mathematik, Humboldt-Universitat zu Berlin Ziegelstr. 13a, D-10099 Berlin, Germany. E-mail: altmann@mathematik.hu-berlin.de Abstract

More information

represented as the dierence of two concave functions. Denote by DC 1 the class of DC-functions on M which are C 1 on the nonsingular set of M. Since t

represented as the dierence of two concave functions. Denote by DC 1 the class of DC-functions on M which are C 1 on the nonsingular set of M. Since t SOBOLEV SPACES, LAPLACIAN, AND HEAT KERNEL ON ALEXANDROV SPACES KAUHIRO KUWAE, YOSHIROH MACHIGASHIRA, AND TAKASHI SHIOYA Abstract. We prove the compactness of the imbedding of the Sobolev space W 1;2 ()

More information

A Representation of Excessive Functions as Expected Suprema

A Representation of Excessive Functions as Expected Suprema A Representation of Excessive Functions as Expected Suprema Hans Föllmer & Thomas Knispel Humboldt-Universität zu Berlin Institut für Mathematik Unter den Linden 6 10099 Berlin, Germany E-mail: foellmer@math.hu-berlin.de,

More information

Scattering for the NLS equation

Scattering for the NLS equation Scattering for the NLS equation joint work with Thierry Cazenave (UPMC) Ivan Naumkin Université Nice Sophia Antipolis February 2, 2017 Introduction. Consider the nonlinear Schrödinger equation with the

More information

The Dirichlet s P rinciple. In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation:

The 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 information

Partial Di erential Equations

Partial Di erential Equations Partial Di erential Equations Alexander Grigorian Universität Bielefeld WS 205/6 2 Contents 0 Introduction 0. Examples of PDEs and their origin.................... 0.. Laplace equation..........................

More information

Markov processes Course note 2. Martingale problems, recurrence properties of discrete time chains.

Markov processes Course note 2. Martingale problems, recurrence properties of discrete time chains. Institute for Applied Mathematics WS17/18 Massimiliano Gubinelli Markov processes Course note 2. Martingale problems, recurrence properties of discrete time chains. [version 1, 2017.11.1] We introduce

More information

Chapter 12. Partial di erential equations Di erential operators in R n. The gradient and Jacobian. Divergence and rotation

Chapter 12. Partial di erential equations Di erential operators in R n. The gradient and Jacobian. Divergence and rotation Chapter 12 Partial di erential equations 12.1 Di erential operators in R n The gradient and Jacobian We recall the definition of the gradient of a scalar function f : R n! R, as @f grad f = rf =,..., @f

More information

CONVERGENCE OF GAUGE METHOD FOR INCOMPRESSIBLE FLOW CHENG WANG AND JIAN-GUO LIU

CONVERGENCE OF GAUGE METHOD FOR INCOMPRESSIBLE FLOW CHENG WANG AND JIAN-GUO LIU MATHEMATICS OF COMPUTATION Volume 69, Number 232, Pages 135{1407 S 0025-571(00)0124-5 Article electronically published on March 24, 2000 CONVERGENCE OF GAUGE METHOD FOR INCOMPRESSIBLE FLOW CHENG WANG AND

More information

Neumann problem: p u = juj N() : p 2 u; in ; u n = ; on : Robin problem: R() : Steklov problem: S() : p u = juj p 2 u; in ; p 2 u jruj n + jujp 2 u =

Neumann problem: p u = juj N() : p 2 u; in ; u n = ; on : Robin problem: R() : Steklov problem: S() : p u = juj p 2 u; in ; p 2 u jruj n + jujp 2 u = EIGENVALUE PROBLEMS FOR THE p-laplacian AN L^E DEPARTMENT OF MATHEMATICS, UNIVERSITY OF UTAH 55 SOUTH 4 EAST SALT LAKE CITY, UT 842, USA Abstract. We study nonlinear eigenvalue problems for the p-laplace

More information

Estimates on fractional higher derivatives of weak solutions for the Navier-Stokes equations

Estimates on fractional higher derivatives of weak solutions for the Navier-Stokes equations Estimates on fractional higher derivatives of weak solutions for the Navier-Stokes equations Kyudong Choi, Alexis F. Vasseur May 6, 20 Abstract We study weak solutions of the 3D Navier-Stokes equations

More information

Tools from Lebesgue integration

Tools from Lebesgue integration Tools from Lebesgue integration E.P. van den Ban Fall 2005 Introduction In these notes we describe some of the basic tools from the theory of Lebesgue integration. Definitions and results will be given

More information

PARTIAL REGULARITY OF BRENIER SOLUTIONS OF THE MONGE-AMPÈRE EQUATION

PARTIAL REGULARITY OF BRENIER SOLUTIONS OF THE MONGE-AMPÈRE EQUATION PARTIAL REGULARITY OF BRENIER SOLUTIONS OF THE MONGE-AMPÈRE EQUATION ALESSIO FIGALLI AND YOUNG-HEON KIM Abstract. Given Ω, Λ R n two bounded open sets, and f and g two probability densities concentrated

More information

THE PRINCIPLE OF LIMITING ABSORPTION FOR THE NON-SELFADJOINT. Hideo Nakazawa. Department of Mathematics, Tokyo Metropolitan University

THE PRINCIPLE OF LIMITING ABSORPTION FOR THE NON-SELFADJOINT. Hideo Nakazawa. Department of Mathematics, Tokyo Metropolitan University THE PRINCIPLE OF LIMITING ABSORPTION FOR THE NON-SELFADJOINT SCHR ODINGER OPERATOR WITH ENERGY DEPENDENT POTENTIAL Hideo Nakazaa Department of Mathematics, Tokyo Metropolitan University. 1.9 1.Introduction

More information

FENGBO HANG AND PAUL C. YANG

FENGBO HANG AND PAUL C. YANG Q CURVATURE ON A CLASS OF 3 ANIFOLDS FENGBO HANG AND PAUL C. YANG Abstract. otivated by the strong maximum principle for Paneitz operator in dimension 5 or higher found in [G] and the calculation of the

More information

2 Section 2 However, in order to apply the above idea, we will need to allow non standard intervals ('; ) in the proof. More precisely, ' and may gene

2 Section 2 However, in order to apply the above idea, we will need to allow non standard intervals ('; ) in the proof. More precisely, ' and may gene Introduction 1 A dierential intermediate value theorem by Joris van der Hoeven D pt. de Math matiques (B t. 425) Universit Paris-Sud 91405 Orsay Cedex France June 2000 Abstract Let T be the eld of grid-based

More information

INSTITUTE OF MATHEMATICS THE CZECH ACADEMY OF SCIENCES. Note on the fast decay property of steady Navier-Stokes flows in the whole space

INSTITUTE OF MATHEMATICS THE CZECH ACADEMY OF SCIENCES. Note on the fast decay property of steady Navier-Stokes flows in the whole space INSTITUTE OF MATHEMATICS THE CZECH ACADEMY OF SCIENCES Note on the fast decay property of stea Navier-Stokes flows in the whole space Tomoyuki Nakatsuka Preprint No. 15-017 PRAHA 017 Note on the fast

More information

Partial Differential Equations, 2nd Edition, L.C.Evans Chapter 5 Sobolev Spaces

Partial Differential Equations, 2nd Edition, L.C.Evans Chapter 5 Sobolev Spaces Partial Differential Equations, nd Edition, L.C.Evans Chapter 5 Sobolev Spaces Shih-Hsin Chen, Yung-Hsiang Huang 7.8.3 Abstract In these exercises always denote an open set of with smooth boundary. As

More information

CRITERIA FOR THE 3D NAVIER-STOKES SYSTEM

CRITERIA FOR THE 3D NAVIER-STOKES SYSTEM LOCAL ENERGY BOUNDS AND ɛ-regularity CRITERIA FOR THE 3D NAVIER-STOKES SYSTEM CRISTI GUEVARA AND NGUYEN CONG PHUC Abstract. The system of three dimensional Navier-Stokes equations is considered. We obtain

More information

Nonexistence results and estimates for some nonlinear elliptic problems

Nonexistence results and estimates for some nonlinear elliptic problems Nonexistence results and estimates for some nonlinear elliptic problems Marie-Francoise BDAUT-VERON Stanislav POHOAEV y. Abstract Here we study the local or global behaviour of the solutions of elliptic

More information

The Erwin Schrodinger International Pasteurgasse 6/7. Institute for Mathematical Physics A-1090 Wien, Austria

The Erwin Schrodinger International Pasteurgasse 6/7. Institute for Mathematical Physics A-1090 Wien, Austria ESI The Erwin Schrodinger International Pasteurgasse 6/7 Institute for Mathematical Physics A-1090 Wien, Austria On the Point Spectrum of Dirence Schrodinger Operators Vladimir Buslaev Alexander Fedotov

More information

Problem Set 2: Solutions Math 201A: Fall 2016

Problem Set 2: Solutions Math 201A: Fall 2016 Problem Set 2: s Math 201A: Fall 2016 Problem 1. (a) Prove that a closed subset of a complete metric space is complete. (b) Prove that a closed subset of a compact metric space is compact. (c) Prove that

More information

Friedrich symmetric systems

Friedrich symmetric systems viii CHAPTER 8 Friedrich symmetric systems In this chapter, we describe a theory due to Friedrich [13] for positive symmetric systems, which gives the existence and uniqueness of weak solutions of boundary

More information

Recent developments in the Navier-Stokes problem

Recent developments in the Navier-Stokes problem P G Lemarie-Rieusset Recent developments in the Navier-Stokes problem CHAPMAN & HALL/CRC A CRC Press Company Boca Raton London New York Washington, D.C. Table of contents Introduction 1 Chapter 1: What

More information

Counterexamples to witness conjectures. Notations Let E be the set of admissible constant expressions built up from Z; + ;?;;/; exp and log. Here a co

Counterexamples to witness conjectures. Notations Let E be the set of admissible constant expressions built up from Z; + ;?;;/; exp and log. Here a co Counterexamples to witness conjectures Joris van der Hoeven D pt. de Math matiques (b t. 45) Universit Paris-Sud 91405 Orsay CEDEX France August 15, 003 Consider the class of exp-log constants, which is

More information

Laplace s Equation. Chapter Mean Value Formulas

Laplace s Equation. Chapter Mean Value Formulas Chapter 1 Laplace s Equation Let be an open set in R n. A function u C 2 () is called harmonic in if it satisfies Laplace s equation n (1.1) u := D ii u = 0 in. i=1 A function u C 2 () is called subharmonic

More information

Thus f is continuous at x 0. Matthew Straughn Math 402 Homework 6

Thus f is continuous at x 0. Matthew Straughn Math 402 Homework 6 Matthew Straughn Math 402 Homework 6 Homework 6 (p. 452) 14.3.3, 14.3.4, 14.3.5, 14.3.8 (p. 455) 14.4.3* (p. 458) 14.5.3 (p. 460) 14.6.1 (p. 472) 14.7.2* Lemma 1. If (f (n) ) converges uniformly to some

More information

2 Ben Schweizer As Hocking describes in [5], a discussion focused on the following question: Can one assume that the dynamic contact angle is a consta

2 Ben Schweizer As Hocking describes in [5], a discussion focused on the following question: Can one assume that the dynamic contact angle is a consta A well-posed model for dynamic contact angles Ben Schweizer February 27, 1998 Abstract We consider uid systems with a free boundary and with a point of contact of the free boundary with a solid wall. We

More information

JORDAN CONTENT. J(P, A) = {m(i k ); I k an interval of P contained in int(a)} J(P, A) = {m(i k ); I k an interval of P intersecting cl(a)}.

JORDAN CONTENT. J(P, A) = {m(i k ); I k an interval of P contained in int(a)} J(P, A) = {m(i k ); I k an interval of P intersecting cl(a)}. JORDAN CONTENT Definition. Let A R n be a bounded set. Given a rectangle (cartesian product of compact intervals) R R n containing A, denote by P the set of finite partitions of R by sub-rectangles ( intervals

More information

A RECURRENCE THEOREM ON THE SOLUTIONS TO THE 2D EULER EQUATION

A RECURRENCE THEOREM ON THE SOLUTIONS TO THE 2D EULER EQUATION ASIAN J. MATH. c 2009 International Press Vol. 13, No. 1, pp. 001 006, March 2009 001 A RECURRENCE THEOREM ON THE SOLUTIONS TO THE 2D EULER EQUATION Y. CHARLES LI Abstract. In this article, I will prove

More information

Second order sucient optimality condition for a. nonlinear elliptic control problem. Eduardo Casas and Fredi Troltzsch and Andreas Unger

Second order sucient optimality condition for a. nonlinear elliptic control problem. Eduardo Casas and Fredi Troltzsch and Andreas Unger Second order sucient optimality condition for a nonlinear elliptic control problem by Eduardo Casas and Fredi Troltzsch and Andreas Unger Technical University of Chemnitz wickau Faculty of Mathematics

More information

A MULTIGRID ALGORITHM FOR. Richard E. Ewing and Jian Shen. Institute for Scientic Computation. Texas A&M University. College Station, Texas SUMMARY

A MULTIGRID ALGORITHM FOR. Richard E. Ewing and Jian Shen. Institute for Scientic Computation. Texas A&M University. College Station, Texas SUMMARY A MULTIGRID ALGORITHM FOR THE CELL-CENTERED FINITE DIFFERENCE SCHEME Richard E. Ewing and Jian Shen Institute for Scientic Computation Texas A&M University College Station, Texas SUMMARY In this article,

More information

Scientiae Mathematicae Japonicae Online, Vol. 5, (2001), Ryo Ikehata Λ and Tokio Matsuyama y

Scientiae Mathematicae Japonicae Online, Vol. 5, (2001), Ryo Ikehata Λ and Tokio Matsuyama y Scientiae Mathematicae Japonicae Online, Vol. 5, (2), 7 26 7 L 2 -BEHAVIOUR OF SOLUTIONS TO THE LINEAR HEAT AND WAVE EQUATIONS IN EXTERIOR DOMAINS Ryo Ikehata Λ and Tokio Matsuyama y Received November

More information

MATH 31BH Homework 1 Solutions

MATH 31BH Homework 1 Solutions MATH 3BH Homework Solutions January 0, 04 Problem.5. (a) (x, y)-plane in R 3 is closed and not open. To see that this plane is not open, notice that any ball around the origin (0, 0, 0) will contain points

More information

ON THE ASYMPTOTIC BEHAVIOR OF THE PRINCIPAL EIGENVALUES OF SOME ELLIPTIC PROBLEMS

ON THE ASYMPTOTIC BEHAVIOR OF THE PRINCIPAL EIGENVALUES OF SOME ELLIPTIC PROBLEMS ON THE ASYMPTOTIC BEHAVIOR OF THE PRINCIPAL EIGENVALUES OF SOME ELLIPTIC PROBLEMS TOMAS GODOY, JEAN-PIERRE GOSSE, AND SOFIA PACKA Abstract. This paper is concerned with nonselfadjoint elliptic problems

More information

STOCHASTIC DIFFERENTIAL EQUATIONS WITH EXTRA PROPERTIES H. JEROME KEISLER. Department of Mathematics. University of Wisconsin.

STOCHASTIC DIFFERENTIAL EQUATIONS WITH EXTRA PROPERTIES H. JEROME KEISLER. Department of Mathematics. University of Wisconsin. STOCHASTIC DIFFERENTIAL EQUATIONS WITH EXTRA PROPERTIES H. JEROME KEISLER Department of Mathematics University of Wisconsin Madison WI 5376 keisler@math.wisc.edu 1. Introduction The Loeb measure construction

More information

Basic Proof Techniques

Basic Proof Techniques Basic Proof Techniques Joshua Wilde, revised by Isabel Tecu, Takeshi Suzuki and María José Boccardi August 13, 2013 1 Basic Notation The following is standard notation for proofs: A B. A implies B. A B.

More information

Math 413/513 Chapter 6 (from Friedberg, Insel, & Spence)

Math 413/513 Chapter 6 (from Friedberg, Insel, & Spence) Math 413/513 Chapter 6 (from Friedberg, Insel, & Spence) David Glickenstein December 7, 2015 1 Inner product spaces In this chapter, we will only consider the elds R and C. De nition 1 Let V be a vector

More information

Garrett: `Bernstein's analytic continuation of complex powers' 2 Let f be a polynomial in x 1 ; : : : ; x n with real coecients. For complex s, let f

Garrett: `Bernstein's analytic continuation of complex powers' 2 Let f be a polynomial in x 1 ; : : : ; x n with real coecients. For complex s, let f 1 Bernstein's analytic continuation of complex powers c1995, Paul Garrett, garrettmath.umn.edu version January 27, 1998 Analytic continuation of distributions Statement of the theorems on analytic continuation

More information

Math 421, Homework #7 Solutions. We can then us the triangle inequality to find for k N that (x k + y k ) (L + M) = (x k L) + (y k M) x k L + y k M

Math 421, Homework #7 Solutions. We can then us the triangle inequality to find for k N that (x k + y k ) (L + M) = (x k L) + (y k M) x k L + y k M Math 421, Homework #7 Solutions (1) Let {x k } and {y k } be convergent sequences in R n, and assume that lim k x k = L and that lim k y k = M. Prove directly from definition 9.1 (i.e. don t use Theorem

More information

Rearrangement on Conditionally Convergent Integrals in Analogy to Series

Rearrangement on Conditionally Convergent Integrals in Analogy to Series Electronic Proceedings of Undergraduate Mathematics Day, Vol. 3 (8), No. 6 Rearrangement on Conditionally Convergent Integrals in Analogy to Series Edward J Timko University of Dayton Dayton OH 45469-36

More information

is a weak solution with the a ij,b i,c2 C 1 ( )

is a weak solution with the a ij,b i,c2 C 1 ( ) Thus @u @x i PDE 69 is a weak solution with the RHS @f @x i L. Thus u W 3, loc (). Iterating further, and using a generalized Sobolev imbedding gives that u is smooth. Theorem 3.33 (Local smoothness).

More information

Heat kernels of some Schrödinger operators

Heat kernels of some Schrödinger operators Heat kernels of some Schrödinger operators Alexander Grigor yan Tsinghua University 28 September 2016 Consider an elliptic Schrödinger operator H = Δ + Φ, where Δ = n 2 i=1 is the Laplace operator in R

More information

Research Article Remarks on the Regularity Criterion of the Navier-Stokes Equations with Nonlinear Damping

Research Article Remarks on the Regularity Criterion of the Navier-Stokes Equations with Nonlinear Damping Mathematical Problems in Engineering Volume 15, Article ID 194, 5 pages http://dx.doi.org/1.1155/15/194 Research Article Remarks on the Regularity Criterion of the Navier-Stokes Equations with Nonlinear

More information

Universität des Saarlandes. Fachrichtung 6.1 Mathematik

Universität des Saarlandes. Fachrichtung 6.1 Mathematik Universität des Saarlandes U N I V E R S I T A S S A R A V I E N I S S Fachrichtung 6.1 Mathematik Preprint Nr. 166 A short remark on energy functionals related to nonlinear Hencky materials Michael Bildhauer

More information

1 Dieses Skriptum ist fur eine summer{school entstanden, die im August 1993 an der Universitat Jyvaskyla, Finnland, stattgefunden hat. Es wird in die

1 Dieses Skriptum ist fur eine summer{school entstanden, die im August 1993 an der Universitat Jyvaskyla, Finnland, stattgefunden hat. Es wird in die Linear Elliptic Boundary Value Problems of Second Order Karl{Josef Witsch Fachbereich 6 Mathematik und Informatik der Universitat GH Essen 45117 Essen August 1993 1 Dieses Skriptum ist fur eine summer{school

More information

Title: Localized self-adjointness of Schrödinger-type operators on Riemannian manifolds. Proposed running head: Schrödinger-type operators on

Title: Localized self-adjointness of Schrödinger-type operators on Riemannian manifolds. Proposed running head: Schrödinger-type operators on Title: Localized self-adjointness of Schrödinger-type operators on Riemannian manifolds. Proposed running head: Schrödinger-type operators on manifolds. Author: Ognjen Milatovic Department Address: Department

More information

GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS

GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS LE MATEMATICHE Vol. LI (1996) Fasc. II, pp. 335347 GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS CARLO SBORDONE Dedicated to Professor Francesco Guglielmino on his 7th birthday W

More information

Some nonlinear elliptic equations in R N

Some nonlinear elliptic equations in R N Nonlinear Analysis 39 000) 837 860 www.elsevier.nl/locate/na Some nonlinear elliptic equations in Monica Musso, Donato Passaseo Dipartimento di Matematica, Universita di Pisa, Via Buonarroti,, 5617 Pisa,

More information

Minimization problems on the Hardy-Sobolev inequality

Minimization problems on the Hardy-Sobolev inequality manuscript No. (will be inserted by the editor) Minimization problems on the Hardy-Sobolev inequality Masato Hashizume Received: date / Accepted: date Abstract We study minimization problems on Hardy-Sobolev

More information

The Erwin Schrodinger International Boltzmanngasse 9. Institute for Mathematical Physics A-1090 Wien, Austria

The Erwin Schrodinger International Boltzmanngasse 9. Institute for Mathematical Physics A-1090 Wien, Austria ESI The Erwin Schrodinger International Boltzmanngasse 9 Institute for Mathematical Physics A-090 Wien, Austria Lipschitz Image of a Measure{null Set Can Have a Null Complement J. Lindenstrauss E. Matouskova

More information

Supplement. The Extended Complex Plane

Supplement. The Extended Complex Plane The Extended Complex Plane 1 Supplement. The Extended Complex Plane Note. In section I.6, The Extended Plane and Its Spherical Representation, we introduced the extended complex plane, C = C { }. We defined

More information

Math 699 Reading Course, Spring 2007 Rouben Rostamian Homogenization of Differential Equations May 11, 2007 by Alen Agheksanterian

Math 699 Reading Course, Spring 2007 Rouben Rostamian Homogenization of Differential Equations May 11, 2007 by Alen Agheksanterian . Introduction Math 699 Reading Course, Spring 007 Rouben Rostamian Homogenization of ifferential Equations May, 007 by Alen Agheksanterian In this brief note, we will use several results from functional

More information

Real Analysis, 2nd Edition, G.B.Folland Signed Measures and Differentiation

Real Analysis, 2nd Edition, G.B.Folland Signed Measures and Differentiation Real Analysis, 2nd dition, G.B.Folland Chapter 3 Signed Measures and Differentiation Yung-Hsiang Huang 3. Signed Measures. Proof. The first part is proved by using addivitiy and consider F j = j j, 0 =.

More information

1 Which sets have volume 0?

1 Which sets have volume 0? Math 540 Spring 0 Notes #0 More on integration Which sets have volume 0? The theorem at the end of the last section makes this an important question. (Measure theory would supersede it, however.) Theorem

More information

ANDREA TOSELLI. Abstract. Two-level overlapping Schwarz methods are considered for nite element problems

ANDREA TOSELLI. Abstract. Two-level overlapping Schwarz methods are considered for nite element problems OVERLAPPING SCHWARZ METHODS FOR MAXWELL'S EQUATIONS IN THREE DIMENSIONS ANDREA TOSELLI Abstract. Two-level overlapping Schwarz methods are considered for nite element problems of 3D Maxwell's equations.

More information

ADDENDUM B: CONSTRUCTION OF R AND THE COMPLETION OF A METRIC SPACE

ADDENDUM B: CONSTRUCTION OF R AND THE COMPLETION OF A METRIC SPACE ADDENDUM B: CONSTRUCTION OF R AND THE COMPLETION OF A METRIC SPACE ANDREAS LEOPOLD KNUTSEN Abstract. These notes are written as supplementary notes for the course MAT11- Real Analysis, taught at the University

More information

5.3. Compactness results for Dirichlet spaces Compactness results for manifolds 39 References 39 sec:intro 1. Introduction We mean by a spectr

5.3. Compactness results for Dirichlet spaces Compactness results for manifolds 39 References 39 sec:intro 1. Introduction We mean by a spectr CONVERGENCE OF SPECTRAL STRUCTURES: A FUNCTIONAL ANALYTIC THEORY AND ITS APPLICATIONS TO SPECTRAL GEOMETRY KAZUHIRO KUWAE AND TAKASHI SHIOYA Abstract. The purpose of this paper is to present a functional

More information

2 JUNCHENG WEI Lin, Ni and Takagi rst in [11] established the existence of leastenergy solutions and Ni and Takagi in [13] and [14] showed that for su

2 JUNCHENG WEI Lin, Ni and Takagi rst in [11] established the existence of leastenergy solutions and Ni and Takagi in [13] and [14] showed that for su UNIQUENESS AND EIGENVALUE ESTIMATES OF BOUNDARY SPIKE SOLUTIONS JUNCHENG WEI Abstract. We study the properties of single boundary spike solutions for the following singularly perturbed problem 2 u? u +

More information

p (z) = p z 1 pz : The pseudo-hyperbolic distance ½(z; w) between z and w in D is de ned by ½(z; w) = j z (w)j =

p (z) = p z 1 pz : The pseudo-hyperbolic distance ½(z; w) between z and w in D is de ned by ½(z; w) = j z (w)j = EXTREME POINTS OF THE CLOSED CONVEX HULL OF COMPOSITION OPERATORS TAKUYA HOSOKAW A Abstract. W e study the extreme points of the closed convex hull of the set of all composition operators on the space

More information

DETERMINATION OF THE BLOW-UP RATE FOR THE SEMILINEAR WAVE EQUATION

DETERMINATION OF THE BLOW-UP RATE FOR THE SEMILINEAR WAVE EQUATION DETERMINATION OF THE LOW-UP RATE FOR THE SEMILINEAR WAVE EQUATION y FRANK MERLE and HATEM ZAAG Abstract. In this paper, we find the optimal blow-up rate for the semilinear wave equation with a power nonlinearity.

More information

Minimum and maximum values *

Minimum and maximum values * OpenStax-CNX module: m17417 1 Minimum and maximum values * Sunil Kumar Singh This work is produced by OpenStax-CNX and licensed under the Creative Commons Attribution License 2.0 In general context, a

More information

A generalised Ladyzhenskaya inequality and a coupled parabolic-elliptic problem

A 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 information

Sobolev Spaces. Chapter Hölder spaces

Sobolev Spaces. Chapter Hölder spaces Chapter 2 Sobolev Spaces Sobolev spaces turn out often to be the proper setting in which to apply ideas of functional analysis to get information concerning partial differential equations. Here, we collect

More information

arxiv: v1 [math.ap] 28 Mar 2014

arxiv: v1 [math.ap] 28 Mar 2014 GROUNDSTATES OF NONLINEAR CHOQUARD EQUATIONS: HARDY-LITTLEWOOD-SOBOLEV CRITICAL EXPONENT VITALY MOROZ AND JEAN VAN SCHAFTINGEN arxiv:1403.7414v1 [math.ap] 28 Mar 2014 Abstract. We consider nonlinear Choquard

More information

Winter Lecture 10. Convexity and Concavity

Winter Lecture 10. Convexity and Concavity Andrew McLennan February 9, 1999 Economics 5113 Introduction to Mathematical Economics Winter 1999 Lecture 10 Convexity and Concavity I. Introduction A. We now consider convexity, concavity, and the general

More information

Functional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability...

Functional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability... Functional Analysis Franck Sueur 2018-2019 Contents 1 Metric spaces 1 1.1 Definitions........................................ 1 1.2 Completeness...................................... 3 1.3 Compactness......................................

More information

University of Cyprus. Abstract. singularities is analyzed. In this method, the solution is approximated by the

University of Cyprus. Abstract. singularities is analyzed. In this method, the solution is approximated by the A Singular Function Boundary Integral Method for Elliptic Problems with Singularities hristos Xenophontos, Miltiades Elliotis and Georgios Georgiou Department of Mathematics and Statistics University of

More information

COMPACTNESS IN L 1, DUNFORD-PETTIS OPERATORS, GEOMETRY OF BANACH SPACES Maria Girardi University of Illinois at Urbana-Champaign Proc. Amer. Math. Soc

COMPACTNESS IN L 1, DUNFORD-PETTIS OPERATORS, GEOMETRY OF BANACH SPACES Maria Girardi University of Illinois at Urbana-Champaign Proc. Amer. Math. Soc COMPCTNESS IN L 1, DUNFOD-PETTIS OPETOS, GEOMETY OF NCH SPCES Maria Girardi University of Illinois at Urbana-Champaign Proc. mer. Math. Soc. 111 (1991) 767{777 bstract. type of oscillation modeled on MO

More information

The Incompressible Navier Stokes Flow in Two Dimensions with Prescribed Vorticity

The Incompressible Navier Stokes Flow in Two Dimensions with Prescribed Vorticity The Incompressible Navier Stokes Flow in Two Dimensions with Prescribed Vorticity Sagun Chanillo, Jean Van Schaftingen, and Po-Lam Yung To Dick Wheeden in friendship and appreciation Abstract We study

More information

Dissipative quasi-geostrophic equations with L p data

Dissipative quasi-geostrophic equations with L p data Electronic Journal of Differential Equations, Vol. (), No. 56, pp. 3. ISSN: 7-669. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) Dissipative quasi-geostrophic

More information

if <v;w>=0. The length of a vector v is kvk, its distance from 0. If kvk =1,then v is said to be a unit vector. When V is a real vector space, then on

if <v;w>=0. The length of a vector v is kvk, its distance from 0. If kvk =1,then v is said to be a unit vector. When V is a real vector space, then on Function Spaces x1. Inner products and norms. From linear algebra, we recall that an inner product for a complex vector space V is a function < ; >: VV!C that satises the following properties. I1. Positivity:

More information

Functions: A Fourier Approach. Universitat Rostock. Germany. Dedicated to Prof. L. Berg on the occasion of his 65th birthday.

Functions: A Fourier Approach. Universitat Rostock. Germany. Dedicated to Prof. L. Berg on the occasion of his 65th birthday. Approximation Properties of Multi{Scaling Functions: A Fourier Approach Gerlind Plona Fachbereich Mathemati Universitat Rostoc 1851 Rostoc Germany Dedicated to Prof. L. Berg on the occasion of his 65th

More information

Stanford Mathematics Department Math 205A Lecture Supplement #4 Borel Regular & Radon Measures

Stanford Mathematics Department Math 205A Lecture Supplement #4 Borel Regular & Radon Measures 2 1 Borel Regular Measures We now state and prove an important regularity property of Borel regular outer measures: Stanford Mathematics Department Math 205A Lecture Supplement #4 Borel Regular & Radon

More information

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 21, 2003, 211 226 SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS Massimo Grosi Filomena Pacella S.

More information

Math 117: Topology of the Real Numbers

Math 117: Topology of the Real Numbers Math 117: Topology of the Real Numbers John Douglas Moore November 10, 2008 The goal of these notes is to highlight the most important topics presented in Chapter 3 of the text [1] and to provide a few

More information

Axioms of Adaptivity (AoA) in Lecture 2 (sufficient for optimal convergence rates)

Axioms of Adaptivity (AoA) in Lecture 2 (sufficient for optimal convergence rates) Axioms of Adaptivity (AoA) in Lecture 2 (sufficient for optimal convergence rates) Carsten Carstensen Humboldt-Universität zu Berlin 2018 International Graduate Summer School on Frontiers of Applied and

More information

LEBESGUE INTEGRATION. Introduction

LEBESGUE INTEGRATION. Introduction LEBESGUE INTEGATION EYE SJAMAA Supplementary notes Math 414, Spring 25 Introduction The following heuristic argument is at the basis of the denition of the Lebesgue integral. This argument will be imprecise,

More information

212a1214Daniell s integration theory.

212a1214Daniell s integration theory. 212a1214 Daniell s integration theory. October 30, 2014 Daniell s idea was to take the axiomatic properties of the integral as the starting point and develop integration for broader and broader classes

More information

Gerhard Rein. Mathematisches Institut der Universitat Munchen, Alan D. Rendall. Max-Planck-Institut fur Astrophysik, and

Gerhard Rein. Mathematisches Institut der Universitat Munchen, Alan D. Rendall. Max-Planck-Institut fur Astrophysik, and A regularity theorem for solutions of the spherically symmetric Vlasov-Einstein system Gerhard Rein Mathematisches Institut der Universitat Munchen, Theresienstr. 39, 80333 Munchen, Germany, Alan D. Rendall

More information