Maximum Principles for Parabolic Equations
|
|
- Buck Oliver
- 5 years ago
- Views:
Transcription
1 Maximum Principles for Parabolic Equations Kamyar Malakpoor 24 November 2004 Textbooks: Friedman, A. Partial Differential Equations of Parabolic Type; Protter, M. H, Weinberger, H. F, Maximum Principles in Differential Equations; 1/22
2 Outline Review of MP for the elliptic equations; MP for the heat equation L(u) = 2 u x u 2 t Weak MP for the parabolic equations; Applications; Comparison Principle; Uniqueness Results; Strong MP for the parabolic equations; 2/22
3 Review of MP for the elliptic equations Consider the operator n 2 u Lu a ij (x) + x i x j i,j=1 n i=1 b i (x) u x i + c(x)u (1) in an n-dimensional domain Ω (open and bounded). (A) We say that L is elliptic in Ω, if there exists λ > 0 such that for every x Ω and for any real vector ξ 0, n a ij (x)ξ i ξ j > λ ξ 2 i,j=1 (B) We assume that the coefficients in L are bounded and continuous functions in D 3/22
4 Lu n 2 u a ij (x) + x i x j i,j=1 n i=1 b i (x) u x i + c(x)u A,B c = 0 u C 2 (Ω) C(Ω) and Lu 0 in Ω = supu = max u = max u Ω Ω Ω Weak A,B c 0 u C 2 (Ω) C(Ω) and Lu 0 in Ω = supu = max u max u + Ω Ω Ω u + = max(u,0) MP-elliptic A,B c = 0 Ω Open, bounded and connected, if Lu 0 and u attains maximum at an interior point, = u constant in Ω Strong A,B c 0 Ω Open, bounded and connected, if Lu 0 and u attains a non-negative maximum, = u constant in Ω 4/22
5 MP for the Heat Equation L(u) = 2 u x 2 u t Suppose u(x, t) satisfies the inequality L(u) > 0 in the rectangular region = (0, l) (0, T ] then u cannot have a (local) maximum at any interior point. For at such a point 2 u x t 0 and u t = 0, thereby violating Lu > 0 (0,T) S 4 S 1 S 3 S 2 (l,0) x 5/22
6 Suppose u(x, t) satisfies in L(u) 0 in. Then max u = max S 1 S 2 S 3 u Define M := max u. S 1 S 2 S 3 Let (x 0, t 0 ), such that M 1 =: u(x 0, t 0 ) > M. Define v(x) := u(x) + M 1 M (x x 2l 2 0 ) 2, then v(x) < M 1 on S 1 S 2 S 3 and v(x 0, t 0 ) = M 1, Furthermore L(v) = L(u) + M 1 M > 0 on v cannot have an interior maximum. At a maximum on S 4, 2 v/ x 2 0 and therefore v/ t < 0 and this contradicts with u(x 0, t 0 ) = v(x 0, t 0 ) < M. l 2 6/22
7 Weak MP for the Parabolic Equations Consider the operator n 2 u Lu a ij (x, t) + x i x j n b i (x, t) u + c(x, t)u x i,j=1 i=1 i }{{} Au u t in = Ω (0, T ], with T > 0, and Ω domain in R n, (open and bounded). (A) We say that L is parabolic in, if there exists λ > 0 such that for every (x, t) and for any real vector ξ 0, n a ij (x, t)ξ i ξ j > λ ξ 2 i,j=1 (2) (B) We assume that the coefficients in L are bounded functions in 7/22
8 Weak MP for the Parabolic Equations(1) Lu Notation: n 2 u n a ij (x, t) + x i,j=1 i x j i=1 }{{} Au b i (x, t) u x i + c(x, t)u C (2,1) ( ) = {u : R; u, u t, u x i, Define = Ω {T }. u t 2 u x i x j C( )} Theorem: Let (A),(B) hold and c = 0. If u C (2,1) ( ) C( ) satisfies L(u) = A(u) u t 0, then sup u = max u = max u 8/22
9 Proof. Suppose L(u) > 0 and max is attained at (x 0, t 0 ). Therefore u/ x i = u/ t = 0 at (x 0, t 0 ) and D 2 u := ( 2 u x i x j (x 0, t 0 )) i,j is negative semi-definite, therefore 0 <L(u) = (a ij ) : D 2 (u) 0, contradiction!! If the max is attained at (x 0, T ), then u/ t(x 0, T ) 0 0 <L(u) = (a ij ) : D 2 (u) u t 0, contradiction!! If L(u) 0, then take u ɛ = u ɛt L(u ɛ ) = (A t )(u ɛt) = L(u) + ɛ > 0 This implies that max u ɛ = max u ɛ for every ɛ > 0. The assertion follows as ɛ 0. 9/22
10 Weak MP for the Parabolic Equations(2) Lu n 2 u n a ij (x, t) + x i,j=1 i x j i=1 }{{} Au b i (x, t) u x i + c(x, t)u u t Theorem: Let (A),(B) hold and c 0 implies that, if u C (2,1) ( ) C( ) satisfies L(u) = A(u) u t 0, then sup u = max u max u + where u = u + u, u + = max(u, 0). 10/22
11 Proof. Suppose L(u) > 0, and that u has a nonnegative maximum at (x 0, t 0 ), then 0<L(u) = ((a ij ) : D 2 (u) + c(x }{{} 0, t 0 )) }{{}}{{} u , contradiction!! If the max is attained at (x 0, T ), then u/ t(x 0, T ) 0 0 <L(u) = (a ij ) : D 2 (u) }{{} 0 u t }{{} 0 + c(x 0, T )u }{{} 0 0, contradiction!! 11/22
12 Proof. If L(u) 0. Suppose Ω { x 1 < d}. Consider u ɛ = u + ɛe αx 1 L(u ɛ ) = (A t )(u + ɛe αx 1 ) = L(u) + ɛ(α 2 a 11 (x, t) + αb 1 (x, t) + c(x, t))e αx 1 ɛ(α 2 λ α b 1 c )e αx 1. By choosing α large enough, L(u ɛ ) > 0, therefore sup u sup u ɛ max u + ɛ = max u + ɛ max u + + ɛe αd Ω T for every ɛ > 0. The assertion follows as ɛ 0. /22
13 Lu n 2 u a ij (x, t) + x i x j } {{ } Au i,j=1 i=1 Weak A,B c 0 MP-parabolic A,B c = 0 Strong A,B c 0 n b i (x, t) u x i + c(x, t)u u t A,B c = 0 u C (2,1) ( ) C( ) and Lu 0 in = supu = max u = max u u C 2 ( ) C( ) and Lu 0 in = supu = max u max u + u + = max(u,0) 13/22
14 Applications In this section we derive bounds on solution u of the equation L(u) = f in. (1). Let (A) and (B) hold and c(x, t) 0. If L(u) = 0 in, then max u max u (apply the weak MP to u and to u). (2). Let (A) and (B) hold and c(x, t) η. If L(u) = 0 in, then max u e ηt max u (apply (1) to v := ue ηt. Indeed, (A t )(ue ηt ) = e ηt (A(u) t u+ηu). 14/22
15 Applications (Continue) (3). Let (A) and (B) hold and c(x, t) 0. Also assume that Ω { x 1 < d} and a 11 λ 2 +b 1 λ 1 in, for some positive constant λ. If L(u) = f in, then max u max u + (e λd 1)max f define w := ±u max u (1 e λx 1 )eλd max f, then L(w) 0 in Ω, therefore w 0 on, and this results the above inequality. 15/22
16 Applications (Continue) (4). If in (3) the assumption c(x, t) 0 replaced by c(x, t) η, then [ ] max u e ηt max u This follows by applying (3) to v := ue ηt. + (e λd 1)max f 16/22
17 Comparison Principle Theorem. Let (A) and (B) hold. Let c 0 and suppose that f(x, t, u) is a continuous function of variables x, t and u and satisfies the one-sided uniform Lipschitz condition in u f(x, t, v) f(x, t, u) k(v u), x, t, u, v, v > u, If u, v C (2,1) ( ) C( ) satisfy Lu + f(x, t, u) 0 and Lv + f(x, t, v) 0 in, and u v in, then u v, in. Proof. 0 L(u v)+f(x, t, u) f(x, t, v) (L+k)(u v), therefore max(u v) e (k+ c T ) max(u v) 0 17/22
18 Uniqueness Results The First initial boundary value problem consists of solving the differential equation Lu(x, t) = f(x, t), in ; u(x, 0) = ϕ(x), on Ω {0}; u(x, t) = g(x, t), on Ω (0, T ]. Theorem. Let (A) and (B) hold. Then there exists at most one solution to the above problem. Proof. The assumption (B) implies that c(x, t) is bounded, c(x, t) η. Define v := ue ηt. This transformation carries Lu = 0 into Lv := Lv ηv = 0. Now the assertion of the theorem follows from the weak MP for v and v. 18/22
19 Nonlinear Parabolic Equations Consider the nonlinear differential operator Lu F (x, t, u, u x i, 2 u ) u x i x j t, where F is a nonlinear function of its arguments. We say that F is parabolic at a point (x 0, t 0 ) if for any p, p 1,, p n, p 11,, p nn, the matrix ( ) F (x0, t 0, p, p i, p ii ) is positive definite. p hk If Lu 1 = Lu 2 in the domain then, by the mean value theorem, 19/22
20 (u 1 u 2 ) t = F (x, t, u 1, u1 2 u 1, ) F (x, t, u 2, u2 2 u 2, ) x i x i x j x i x i x j = 2 (u 1 u 2 ) a hk + (u 1 u 2 ) b h + c(u 1 u 2 ), x h x k x h where a hk, b h, c are continuous functions provided F/ p, F/ p h, F/ p h k are continuous functions. (a hk ) is positive definite matrix. Applying the previous theorem, we conclude that there exists at most one solution to Lu = 0. 20/22
21 Strong MP for the Parabolic Equations Theorem. Let Ω be open, bounded, and connected in R n. Let (A) and (B) hold. Let u C (1,2) ( ) C( ) with Lu = Au t u 0, then If c 0, then u cannot have a global maximum in, unless u is constant. If c 0, then u cannot have a global nonnegative maximum in, unless u is constant. 21/22
22 Lu n 2 u a ij (x, t) + x i,j=1 i x j i=1 }{{} Au n b i (x, t) u x i + c(x, t)u u t A,B c = 0 u C (2,1) ( ) C( ) and Lu 0 in = supu = max u = max u Weak A,B c 0 u C 2 ( ) C( ) and Lu 0 in = supu = max u max u + u + = max(u,0) MP-parabolic A,B c = 0 ΩT Open, bounded and connected, if Lu 0 and u attains maximum at an interior point, = u constant in Strong A,B c 0 Open, bounded and connected, if Lu 0 and u attains a non-negative maximum, = u constant in 22/22
Remarks on the Maximum Principle for Parabolic-Type PDEs
International Mathematical Forum, Vol. 11, 2016, no. 24, 1185-1190 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/imf.2016.69125 Remarks on the Maximum Principle for Parabolic-Type PDEs Humberto
More informationMaximum Principles for Elliptic and Parabolic Operators
Maximum Principles for Elliptic and Parabolic Operators Ilia Polotskii 1 Introduction Maximum principles have been some of the most useful properties used to solve a wide range of problems in the study
More informationKrein-Rutman Theorem and the Principal Eigenvalue
Chapter 1 Krein-Rutman Theorem and the Principal Eigenvalue The Krein-Rutman theorem plays a very important role in nonlinear partial differential equations, as it provides the abstract basis for the proof
More informationAhmed Mohammed. Harnack Inequality for Non-divergence Structure Semi-linear Elliptic Equations
Harnack Inequality for Non-divergence Structure Semi-linear Elliptic Equations International Conference on PDE, Complex Analysis, and Related Topics Miami, Florida January 4-7, 2016 An Outline 1 The Krylov-Safonov
More informationANALYSIS AND APPLICATION OF DIFFUSION EQUATIONS INVOLVING A NEW FRACTIONAL DERIVATIVE WITHOUT SINGULAR KERNEL
Electronic Journal of Differential Equations, Vol. 217 (217), No. 289, pp. 1 6. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ANALYSIS AND APPLICATION OF DIFFUSION EQUATIONS
More informationThe continuity method
The continuity method The method of continuity is used in conjunction with a priori estimates to prove the existence of suitably regular solutions to elliptic partial differential equations. One crucial
More informationOblique derivative problems for elliptic and parabolic equations, Lecture II
of the for elliptic and parabolic equations, Lecture II Iowa State University July 22, 2011 of the 1 2 of the of the As a preliminary step in our further we now look at a special situation for elliptic.
More informationA Perron-type theorem on the principal eigenvalue of nonsymmetric elliptic operators
A Perron-type theorem on the principal eigenvalue of nonsymmetric elliptic operators Lei Ni And I cherish more than anything else the Analogies, my most trustworthy masters. They know all the secrets of
More informationA metric space X is a non-empty set endowed with a metric ρ (x, y):
Chapter 1 Preliminaries References: Troianiello, G.M., 1987, Elliptic differential equations and obstacle problems, Plenum Press, New York. Friedman, A., 1982, Variational principles and free-boundary
More informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University Numerical Methods for Partial Differential Equations Finite Difference Methods
More informationu(0) = u 0, u(1) = u 1. To prove what we want we introduce a new function, where c = sup x [0,1] a(x) and ɛ 0:
6. Maximum Principles Goal: gives properties of a solution of a PDE without solving it. For the two-point boundary problem we shall show that the extreme values of the solution are attained on the boundary.
More informationFinite difference method for elliptic problems: I
Finite difference method for elliptic problems: I Praveen. C praveen@math.tifrbng.res.in Tata Institute of Fundamental Research Center for Applicable Mathematics Bangalore 560065 http://math.tifrbng.res.in/~praveen
More informationMaximum Principles and the Method of Moving Planes
Maximum Principles and the Method of Moving Planes Wenxiong Chen and Congming Li May 25, 2007 Index 1. Introduction 2. Weak Maximum Principle 3. The Hopf Lemma and Strong Maximum Principle 4. Maximum Principle
More informationCLASSIFICATION AND PRINCIPLE OF SUPERPOSITION FOR SECOND ORDER LINEAR PDE
CLASSIFICATION AND PRINCIPLE OF SUPERPOSITION FOR SECOND ORDER LINEAR PDE 1. Linear Partial Differential Equations A partial differential equation (PDE) is an equation, for an unknown function u, that
More informationGeometric PDE and The Magic of Maximum Principles. Alexandrov s Theorem
Geometric PDE and The Magic of Maximum Principles Alexandrov s Theorem John McCuan December 12, 2013 Outline 1. Young s PDE 2. Geometric Interpretation 3. Maximum and Comparison Principles 4. Alexandrov
More informationAsymptotic behavior of infinity harmonic functions near an isolated singularity
Asymptotic behavior of infinity harmonic functions near an isolated singularity Ovidiu Savin, Changyou Wang, Yifeng Yu Abstract In this paper, we prove if n 2 x 0 is an isolated singularity of a nonegative
More informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University Discretization of Boundary Conditions Discretization of Boundary Conditions On
More informationVISCOSITY SOLUTIONS. We follow Han and Lin, Elliptic Partial Differential Equations, 5.
VISCOSITY SOLUTIONS PETER HINTZ We follow Han and Lin, Elliptic Partial Differential Equations, 5. 1. Motivation Throughout, we will assume that Ω R n is a bounded and connected domain and that a ij C(Ω)
More informationModule 7: The Laplace Equation
Module 7: The Laplace Equation In this module, we shall study one of the most important partial differential equations in physics known as the Laplace equation 2 u = 0 in Ω R n, (1) where 2 u := n i=1
More informationPDEs for a Metro Ride
PDEs for a Metro Ride Lenya Ryzhik 1 October 30, 2012 1 Department of Mathematics, Stanford University, Stanford CA, 94305, USA; ryzhik@math.stanford.edu 2 Chapter 1 Maximum principle and symmetry of solutions
More informationSobolev spaces, Trace theorems and Green s functions.
Sobolev spaces, Trace theorems and Green s functions. Boundary Element Methods for Waves Scattering Numerical Analysis Seminar. Orane Jecker October 21, 2010 Plan Introduction 1 Useful definitions 2 Distributions
More informationSymmetry of nonnegative solutions of elliptic equations via a result of Serrin
Symmetry of nonnegative solutions of elliptic equations via a result of Serrin P. Poláčik School of Mathematics, University of Minnesota Minneapolis, MN 55455 Abstract. We consider the Dirichlet problem
More informationEXISTENCE, UNIQUENESS AND QUENCHING OF THE SOLUTION FOR A NONLOCAL DEGENERATE SEMILINEAR PARABOLIC PROBLEM
Dynamic Systems and Applications 6 (7) 55-559 EXISTENCE, UNIQUENESS AND QUENCHING OF THE SOLUTION FOR A NONLOCAL DEGENERATE SEMILINEAR PARABOLIC PROBLEM C. Y. CHAN AND H. T. LIU Department of Mathematics,
More informationNUMERICAL SOLUTIONS OF NONLINEAR ELLIPTIC PROBLEM USING COMBINED-BLOCK ITERATIVE METHODS
NUMERICAL SOLUTIONS OF NONLINEAR ELLIPTIC PROBLEM USING COMBINED-BLOCK ITERATIVE METHODS Fang Liu A Thesis Submitted to the University of North Carolina at Wilmington in Partial Fulfillment Of the Requirements
More informationMath 104: Homework 7 solutions
Math 04: Homework 7 solutions. (a) The derivative of f () = is f () = 2 which is unbounded as 0. Since f () is continuous on [0, ], it is uniformly continous on this interval by Theorem 9.2. Hence for
More informationA VARIANT OF HOPF LEMMA FOR SECOND ORDER DIFFERENTIAL INEQUALITIES
A VARIANT OF HOPF LEMMA FOR SECOND ORDER DIFFERENTIAL INEQUALITIES YIFEI PAN AND MEI WANG Abstract. We prove a sequence version of Hopf lemma, which is essentially equivalent to the classical version.
More informationLECTURE # 0 BASIC NOTATIONS AND CONCEPTS IN THE THEORY OF PARTIAL DIFFERENTIAL EQUATIONS (PDES)
LECTURE # 0 BASIC NOTATIONS AND CONCEPTS IN THE THEORY OF PARTIAL DIFFERENTIAL EQUATIONS (PDES) RAYTCHO LAZAROV 1 Notations and Basic Functional Spaces Scalar function in R d, d 1 will be denoted by u,
More informationLOWER AND UPPER SOLUTIONS TO SEMILINEAR BOUNDARY VALUE PROBLEMS: AN ABSTRACT APPROACH. Alessandro Fonda Rodica Toader. 1.
Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder University Centre Volume 38, 2011, 59 93 LOWER AND UPPER SOLUTIONS TO SEMILINEAR BOUNDARY VALUE PROBLEMS: AN ABSTRACT APPROACH
More informationChapter 1. Optimality Conditions: Unconstrained Optimization. 1.1 Differentiable Problems
Chapter 1 Optimality Conditions: Unconstrained Optimization 1.1 Differentiable Problems Consider the problem of minimizing the function f : R n R where f is twice continuously differentiable on R n : P
More informationElementary Theory and Methods for Elliptic Partial Differential Equations. John Villavert
Elementary Theory and Methods for Elliptic Partial Differential Equations John Villavert Contents 1 Introduction and Basic Theory 4 1.1 Harmonic Functions............................... 5 1.1.1 Mean Value
More informationOn second order sufficient optimality conditions for quasilinear elliptic boundary control problems
On second order sufficient optimality conditions for quasilinear elliptic boundary control problems Vili Dhamo Technische Universität Berlin Joint work with Eduardo Casas Workshop on PDE Constrained Optimization
More informationChapter 5 A priori error estimates for nonconforming finite element approximations 5.1 Strang s first lemma
Chapter 5 A priori error estimates for nonconforming finite element approximations 51 Strang s first lemma We consider the variational equation (51 a(u, v = l(v, v V H 1 (Ω, and assume that the conditions
More informationApplied Math Qualifying Exam 11 October Instructions: Work 2 out of 3 problems in each of the 3 parts for a total of 6 problems.
Printed Name: Signature: Applied Math Qualifying Exam 11 October 2014 Instructions: Work 2 out of 3 problems in each of the 3 parts for a total of 6 problems. 2 Part 1 (1) Let Ω be an open subset of R
More informationLecture No 1 Introduction to Diffusion equations The heat equat
Lecture No 1 Introduction to Diffusion equations The heat equation Columbia University IAS summer program June, 2009 Outline of the lectures We will discuss some basic models of diffusion equations and
More informationPartial Differential Equations
Part II Partial Differential Equations Year 2015 2014 2013 2012 2011 2010 2009 2008 2007 2006 2005 2015 Paper 4, Section II 29E Partial Differential Equations 72 (a) Show that the Cauchy problem for u(x,
More informationNOTES ON SCHAUDER ESTIMATES. r 2 x y 2
NOTES ON SCHAUDER ESTIMATES CRISTIAN E GUTIÉRREZ JULY 26, 2005 Lemma 1 If u f in B r y), then ux) u + r2 x y 2 B r y) B r y) f, x B r y) Proof Let gx) = ux) Br y) u r2 x y 2 Br y) f We have g = u + Br
More informationt y n (s) ds. t y(s) ds, x(t) = x(0) +
1 Appendix Definition (Closed Linear Operator) (1) The graph G(T ) of a linear operator T on the domain D(T ) X into Y is the set (x, T x) : x D(T )} in the product space X Y. Then T is closed if its graph
More informationTD M1 EDP 2018 no 2 Elliptic equations: regularity, maximum principle
TD M EDP 08 no Elliptic equations: regularity, maximum principle Estimates in the sup-norm I Let be an open bounded subset of R d of class C. Let A = (a ij ) be a symmetric matrix of functions of class
More informationThe Relativistic Heat Equation
Maximum Principles and Behavior near Absolute Zero Washington University in St. Louis ARTU meeting March 28, 2014 The Heat Equation The heat equation is the standard model for diffusion and heat flow,
More informationDifferential Equations 1 - Second Part The Heat Equation. Lecture Notes th March Università di Padova Roberto Monti
Differential Equations 1 - Second Part The Heat Equation Lecture Notes - 2011-11th March Università di Padova Roberto Monti Contents Chapter 1. Heat Equation 5 1. Introduction 5 2. The foundamental solution
More informationOBSERVABILITY INEQUALITIES AND MEASURABLE SETS J. APRAIZ, L. ESCAURIAZA, G. WANG, AND C. ZHANG
OBSERVABILITY INEQUALITIES AND MEASURABLE SETS J. APRAIZ, L. ESCAURIAZA, G. WANG, AND C. ZHANG Abstract. This paper presents two observability inequalities for the heat equation over 0, T ). In the first
More informationREGULARITY RESULTS FOR THE EQUATION u 11 u 22 = Introduction
REGULARITY RESULTS FOR THE EQUATION u 11 u 22 = 1 CONNOR MOONEY AND OVIDIU SAVIN Abstract. We study the equation u 11 u 22 = 1 in R 2. Our results include an interior C 2 estimate, classical solvability
More informationHESSIAN MEASURES III. Centre for Mathematics and Its Applications Australian National University Canberra, ACT 0200 Australia
HESSIAN MEASURES III Neil S. Trudinger Xu-Jia Wang Centre for Mathematics and Its Applications Australian National University Canberra, ACT 0200 Australia 1 HESSIAN MEASURES III Neil S. Trudinger Xu-Jia
More informationCONVERGENCE BEHAVIOUR OF SOLUTIONS TO DELAY CELLULAR NEURAL NETWORKS WITH NON-PERIODIC COEFFICIENTS
Electronic Journal of Differential Equations, Vol. 2007(2007), No. 46, pp. 1 7. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) CONVERGENCE
More informationTitle. Author(s)Giga, Yoshikazu; Hamamuki, Nao. CitationHokkaido University Preprint Series in Mathematics, Issue Date DOI 10.
Title On a dynamic boundary condition for singular degener Author(s)Giga, Yoshikazu; Hamamuki, Nao CitationHokkaido University Preprint Series in Mathematics, Issue Date 2018-04-28 DOI 10.14943/84298 Doc
More informationNumerical Analysis and Methods for PDE I
Numerical Analysis and Methods for PDE I A. J. Meir Department of Mathematics and Statistics Auburn University US-Africa Advanced Study Institute on Analysis, Dynamical Systems, and Mathematical Modeling
More informationGreen s Functions and Distributions
CHAPTER 9 Green s Functions and Distributions 9.1. Boundary Value Problems We would like to study, and solve if possible, boundary value problems such as the following: (1.1) u = f in U u = g on U, where
More informationA drift approximation for parabolic PDEs with oblique boundary data
A drift approximation for parabolic PDEs with oblique boundary data Damon Alexander and Inwon Kim February 17, 2014 Abstract We consider solutions of a quasi-linear parabolic PDE with zero oblique boundary
More informationHARNACK S INEQUALITY FOR COOPERATIVE WEAKLY COUPLED ELLIPTIC SYSTEMS. Ari Arapostathis
HARNACK S INEQUALITY FOR COOPERATIVE WEAKLY COUPLED ELLIPTIC SYSTEMS Ari Arapostathis Department of Electrical and Computer Engineering The University of Texas at Austin Austin, Texas 78712 Mrinal K. Ghosh
More informationRegularity for Poisson Equation
Regularity for Poisson Equation OcMountain Daylight Time. 4, 20 Intuitively, the solution u to the Poisson equation u= f () should have better regularity than the right hand side f. In particular one expects
More informationDynamic programming using radial basis functions and Shepard approximations
Dynamic programming using radial basis functions and Shepard approximations Oliver Junge, Alex Schreiber Fakultät für Mathematik Technische Universität München Workshop on algorithms for dynamical systems
More information[2] (a) Develop and describe the piecewise linear Galerkin finite element approximation of,
269 C, Vese Practice problems [1] Write the differential equation u + u = f(x, y), (x, y) Ω u = 1 (x, y) Ω 1 n + u = x (x, y) Ω 2, Ω = {(x, y) x 2 + y 2 < 1}, Ω 1 = {(x, y) x 2 + y 2 = 1, x 0}, Ω 2 = {(x,
More informationarxiv: v2 [math.oc] 31 Jul 2017
An unconstrained framework for eigenvalue problems Yunho Kim arxiv:6.09707v [math.oc] 3 Jul 07 May 0, 08 Abstract In this paper, we propose an unconstrained framework for eigenvalue problems in both discrete
More informationAppendix A: Separation theorems in IR n
Appendix A: Separation theorems in IR n These notes provide a number of separation theorems for convex sets in IR n. We start with a basic result, give a proof with the help on an auxiliary result and
More informationSecond Order Elliptic PDE
Second Order Elliptic PDE T. Muthukumar tmk@iitk.ac.in December 16, 2014 Contents 1 A Quick Introduction to PDE 1 2 Classification of Second Order PDE 3 3 Linear Second Order Elliptic Operators 4 4 Periodic
More informationTIME-DEPENDENT DOMAINS FOR NONLINEAR EVOLUTION OPERATORS AND PARTIAL DIFFERENTIAL EQUATIONS
Electronic Journal of Differential Equations, Vol. 2011 (2011), No. 92, pp. 1 30. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu TIME-DEPENDENT
More informationViscosity solutions of elliptic equations in R n : existence and uniqueness results
Viscosity solutions of elliptic equations in R n : existence and uniqueness results Department of Mathematics, ITALY June 13, 2012 GNAMPA School DIFFERENTIAL EQUATIONS AND DYNAMICAL SYSTEMS Serapo (Latina),
More informationChapter 3 Second Order Linear Equations
Partial Differential Equations (Math 3303) A Ë@ Õæ Aë áöß @. X. @ 2015-2014 ú GA JË@ É Ë@ Chapter 3 Second Order Linear Equations Second-order partial differential equations for an known function u(x,
More informationi=1 α i. Given an m-times continuously
1 Fundamentals 1.1 Classification and characteristics Let Ω R d, d N, d 2, be an open set and α = (α 1,, α d ) T N d 0, N 0 := N {0}, a multiindex with α := d i=1 α i. Given an m-times continuously differentiable
More informationSome lecture notes for Math 6050E: PDEs, Fall 2016
Some lecture notes for Math 65E: PDEs, Fall 216 Tianling Jin December 1, 216 1 Variational methods We discuss an example of the use of variational methods in obtaining existence of solutions. Theorem 1.1.
More informationu =0with u(0,x)=f(x), (x) =
PDE LECTURE NOTES, MATH 37A-B 69. Heat Equation The heat equation for a function u : R + R n C is the partial differential equation (.) µ t u =0with u(0,x)=f(x), where f is a given function on R n. By
More informationEquilibria with a nontrivial nodal set and the dynamics of parabolic equations on symmetric domains
Equilibria with a nontrivial nodal set and the dynamics of parabolic equations on symmetric domains J. Földes Department of Mathematics, Univerité Libre de Bruxelles 1050 Brussels, Belgium P. Poláčik School
More informationLocal pointwise a posteriori gradient error bounds for the Stokes equations. Stig Larsson. Heraklion, September 19, 2011 Joint work with A.
Local pointwise a posteriori gradient error bounds for the Stokes equations Stig Larsson Department of Mathematical Sciences Chalmers University of Technology and University of Gothenburg Heraklion, September
More informationThe second-order 1D wave equation
C The second-order D wave equation C. Homogeneous wave equation with constant speed The simplest form of the second-order wave equation is given by: x 2 = Like the first-order wave equation, it responds
More informationIn particular, if A is a square matrix and λ is one of its eigenvalues, then we can find a non-zero column vector X with
Appendix: Matrix Estimates and the Perron-Frobenius Theorem. This Appendix will first present some well known estimates. For any m n matrix A = [a ij ] over the real or complex numbers, it will be convenient
More informationA non-local problem with integral conditions for hyperbolic equations
Electronic Journal of Differential Equations, Vol. 1999(1999), No. 45, pp. 1 6. ISSN: 17-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu ftp ejde.math.unt.edu (login:
More informationGradient estimates for eigenfunctions on compact Riemannian manifolds with boundary
Gradient estimates for eigenfunctions on compact Riemannian manifolds with boundary Xiangjin Xu Department of athematics Johns Hopkins University Baltimore, D 21218 Abstract The purpose of this paper is
More informationNon-divergence Elliptic Equations of Second Order with Unbounded Drift
Unspecified Boo Proceedings Series Dedicated to Nina N. Ural tseva Non-divergence Elliptic Equations of Second Order with Unbounded Drift M. V. Safonov Abstract. We consider uniformly elliptic equations
More informationOptimal Transportation. Nonlinear Partial Differential Equations
Optimal Transportation and Nonlinear Partial Differential Equations Neil S. Trudinger Centre of Mathematics and its Applications Australian National University 26th Brazilian Mathematical Colloquium 2007
More informationL p estimates for parabolic equations in Reifenberg domains
Journal of Functional Analysis 223 (2005) 44 85 www.elsevier.com/locate/jfa L p estimates for parabolic equations in Reifenberg domains Sun-Sig Byun a,, Lihe Wang b,c a Department of Mathematics, Seoul
More informationHomogenization of Neuman boundary data with fully nonlinear operator
Homogenization of Neuman boundary data with fully nonlinear operator Sunhi Choi, Inwon C. Kim, and Ki-Ahm Lee Abstract We study periodic homogenization problems for second-order nonlinear pde with oscillatory
More informationGradient estimates and global existence of smooth solutions to a system of reaction-diffusion equations with cross-diffusion
Gradient estimates and global existence of smooth solutions to a system of reaction-diffusion equations with cross-diffusion Tuoc V. Phan University of Tennessee - Knoxville, TN Workshop in nonlinear PDES
More informationA note on W 1,p estimates for quasilinear parabolic equations
200-Luminy conference on Quasilinear Elliptic and Parabolic Equations and Systems, Electronic Journal of Differential Equations, Conference 08, 2002, pp 2 3. http://ejde.math.swt.edu or http://ejde.math.unt.edu
More informationAsymptotic Properties of Positive Solutions of Parabolic Equations and Cooperative Systems with Dirichlet Boundary Data
Asymptotic Properties of Positive Solutions of Parabolic Equations and Cooperative Systems with Dirichlet Boundary Data A THESIS SUBMITTED TO THE FACULTY OF THE GRADUATE SCHOOL OF THE UNIVERSITY OF MINNESOTA
More informationLaplace 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 informationThe method of lines (MOL) for the diffusion equation
Chapter 1 The method of lines (MOL) for the diffusion equation The method of lines refers to an approximation of one or more partial differential equations with ordinary differential equations in just
More informationFifth Abel Conference : Celebrating the Mathematical Impact of John F. Nash Jr. and Louis Nirenberg
Fifth Abel Conference : Celebrating the Mathematical Impact of John F. Nash Jr. and Louis Nirenberg Some analytic aspects of second order conformally invariant equations Yanyan Li Rutgers University November
More informationarxiv: v2 [math.ap] 12 Apr 2019
A new method of proving a priori bounds for superlinear elliptic PDE arxiv:1904.03245v2 [math.ap] 12 Apr 2019 Boyan SIRAKOV 1 PUC-Rio, Departamento de Matematica, Gavea, Rio de Janeiro - CEP 22451-900,
More information1. Introduction, notation, and main results
Publ. Mat. 62 (2018), 439 473 DOI: 10.5565/PUBLMAT6221805 HOMOGENIZATION OF A PARABOLIC DIRICHLET PROBLEM BY A METHOD OF DAHLBERG Alejandro J. Castro and Martin Strömqvist Abstract: Consider the linear
More informationExact controllability of the superlinear heat equation
Exact controllability of the superlinear heat equation Youjun Xu 1,2, Zhenhai Liu 1 1 School of Mathematical Sciences and Computing Technology, Central South University, Changsha, Hunan 410075, P R China
More informationA posteriori error estimation for elliptic problems
A posteriori error estimation for elliptic problems Praveen. C praveen@math.tifrbng.res.in Tata Institute of Fundamental Research Center for Applicable Mathematics Bangalore 560065 http://math.tifrbng.res.in
More informationHomogeniza*ons in Perforated Domain. Ki Ahm Lee Seoul Na*onal University
Homogeniza*ons in Perforated Domain Ki Ahm Lee Seoul Na*onal University Outline 1. Perforated Domain 2. Neumann Problems (joint work with Minha Yoo; interes*ng discussion with Li Ming Yeh) 3. Dirichlet
More informationDYNAMICS IN 3-SPECIES PREDATOR-PREY MODELS WITH TIME DELAYS. Wei Feng
DISCRETE AND CONTINUOUS Website: www.aimsciences.org DYNAMICAL SYSTEMS SUPPLEMENT 7 pp. 36 37 DYNAMICS IN 3-SPECIES PREDATOR-PREY MODELS WITH TIME DELAYS Wei Feng Mathematics and Statistics Department
More informationu xx + u yy = 0. (5.1)
Chapter 5 Laplace Equation The following equation is called Laplace equation in two independent variables x, y: The non-homogeneous problem u xx + u yy =. (5.1) u xx + u yy = F, (5.) where F is a function
More informationThe Maximum Principles and Symmetry results for Viscosity Solutions of Fully Nonlinear Equations
The Maximum Principles and Symmetry results for Viscosity Solutions of Fully Nonlinear Equations Guozhen Lu and Jiuyi Zhu Abstract. This paper is concerned about maximum principles and radial symmetry
More informationReconstruction Scheme for Active Thermography
Reconstruction Scheme for Active Thermography Gen Nakamura gnaka@math.sci.hokudai.ac.jp Department of Mathematics, Hokkaido University, Japan Newton Institute, Cambridge, Sept. 20, 2011 Contents.1.. Important
More informationSobolev Spaces. Chapter 10
Chapter 1 Sobolev Spaces We now define spaces H 1,p (R n ), known as Sobolev spaces. For u to belong to H 1,p (R n ), we require that u L p (R n ) and that u have weak derivatives of first order in L p
More informationCourse Summary Math 211
Course Summary Math 211 table of contents I. Functions of several variables. II. R n. III. Derivatives. IV. Taylor s Theorem. V. Differential Geometry. VI. Applications. 1. Best affine approximations.
More informationElliptic PDE with natural/critical growth in the gradient
Elliptic PDE with natural/critical growth in the gradient September 15, 2015 Given an elliptic operator Lu = a ij (x) ij u + b i (x) i u + c(x)u, F(D 2 u, Du, u, x) Lu = div(a(x) u) + b i (x) i u + c(x)u,
More informationAsymptotic Behavior of Infinity Harmonic Functions Near an Isolated Singularity
Savin, O., and C. Wang. (2008) Asymptotic Behavior of Infinity Harmonic Functions, International Mathematics Research Notices, Vol. 2008, Article ID rnm163, 23 pages. doi:10.1093/imrn/rnm163 Asymptotic
More informationAsymptotic behavior of the degenerate p Laplacian equation on bounded domains
Asymptotic behavior of the degenerate p Laplacian equation on bounded domains Diana Stan Instituto de Ciencias Matematicas (CSIC), Madrid, Spain UAM, September 19, 2011 Diana Stan (ICMAT & UAM) Nonlinear
More informationHomogenization of the free boundary velocity
Homogenization of the free boundary velocity Inwon C. Kim February 17, 2006 Abstract In this paper we investigate some free boundary problems with space-dependent free boundary velocities. Based on maximum
More informationUNIVERSITY OF MANITOBA
Question Points Score INSTRUCTIONS TO STUDENTS: This is a 6 hour examination. No extra time will be given. No texts, notes, or other aids are permitted. There are no calculators, cellphones or electronic
More informationGas solid reaction with porosity change
Nonlinear Differential Equations, Electron. J. Diff. Eqns., Conf. 5, 2, pp. 247 252 http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu or ejde.math.unt.edu (login: ftp) Gas solid
More informationSome estimates and maximum principles for weakly coupled systems of elliptic PDE
Some estimates and maximum principles for weakly coupled systems of elliptic PDE Boyan Sirakov To cite this version: Boyan Sirakov. Some estimates and maximum principles for weakly coupled systems of elliptic
More informationThe Dirichlet boundary problems for second order parabolic operators satisfying a Carleson condition
The Dirichlet boundary problems for second order parabolic operators satisfying a Martin Dindos Sukjung Hwang University of Edinburgh Satellite Conference in Harmonic Analysis Chosun University, Gwangju,
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 informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University A Framework for Interpolation Error Estimation of Affine Equivalent FEs 1 The
More informationIowa State University. Instructor: Alex Roitershtein Summer Homework #5. Solutions
Math 50 Iowa State University Introduction to Real Analysis Department of Mathematics Instructor: Alex Roitershtein Summer 205 Homework #5 Solutions. Let α and c be real numbers, c > 0, and f is defined
More informationFractional Laplacian
Fractional Laplacian Grzegorz Karch 5ème Ecole de printemps EDP Non-linéaire Mathématiques et Interactions: modèles non locaux et applications Ecole Supérieure de Technologie d Essaouira, du 27 au 30 Avril
More information