Generalized Lax-Milgram theorem in Banach spaces and its application to the mathematical fluid mechanics.

Size: px
Start display at page:

Download "Generalized Lax-Milgram theorem in Banach spaces and its application to the mathematical fluid mechanics."

Transcription

1 Second Italian-Japanese Workshop GEOMETRIC PROPERTIES FOR PARABOLIC AND ELLIPTIC PDE s Cortona, Italy, June 2-24, 211 Generalized Lax-Milgram theorem in Banach spaces and its application to the mathematical fluid mechanics. Hideo KOZONO Mathematical Institute, Tohoku University June 21, 211

2 jointly with Taku YANAGISAWA(Nara Women s Univ.) 1. Introduction Lax-Milgram Theorem. X: Hilbert space a(, ) : X X C: bilinear form (i) (bi-continuity) M > such that a(u, ϕ) M u ϕ, u X, ϕ X, (ii) (coercive estimate) δ > such that δ u 2 a(u, u), u X F X,!u X such that Remark. a(u, ϕ) = F (ϕ), ϕ X. u δ 1 F X.

3 c.f.application. Ω R n : bounded domain, Ω C (E) { Lu = f in Ω, Bu = on Ω, L: elliptic operator, B: boundary operator Example 1; Dirichlet Problem L = + c(x), c(x), Bu = u Dirichlet condition X = H 1 (Ω) a(u, ϕ) = ( u, ϕ) + (cu, ϕ), u, ϕ X Lax-Milgram Theorem F H 1 (Ω) H 1(Ω),!u H 1 (Ω) s. t. ( u, ϕ) + (cu, ϕ) = F, ϕ ϕ H 1 (Ω), i.e., u is a unique weak solution of (E).

4 Example 2; Neumann Problem L = + c(x), c(x) >, Bu = u ν X = H 1 (Ω) a(u, ϕ) = ( u, ϕ) + (cu, ϕ), Neumann condition u, ϕ X Lax-Milgram Theorem F H 1 (Ω),!u H 1 (Ω) s. t. ( u, ϕ) + (cu, ϕ) = F, ϕ ϕ H 1 (Ω), Question. L r -case? Problem. F W 1,r (Ω),!u W 1,r (Ω) s.t. ( u, ϕ) + (cu, ϕ) = F, ϕ ϕ W 1,r (Ω), 1/r + 1/r = 1.

5 Simader s approach (LNM 256, Springer 1972) a(u, ϕ) = ( u, ϕ) + (cu, ϕ), u W 1,r 1,r (Ω), ϕ W (Ω), (i) (bi-continuity) M > s.t. a(u, ϕ) M u W 1,r (Ω) ϕ W 1,r (Ω) (ii) (variational inequality) u W 1,r (Ω) C sup ϕ W 1,r (Ω) u W 1,r 1,r (Ω), ϕ W (Ω); a(u, ϕ) ϕ W 1,r (Ω) F W 1,r (Ω) W 1,r (Ω),!u W 1,r (Ω) s.t., u W 1,r (Ω), a(u, ϕ) = F, ϕ, ϕ W 1,r (Ω) The same for the 2m-order elliptic boundary value problem.

6 2. Generalized Lax-Milgram Theorem. (X, X ), (Y, Y ): Banach spaces a(, ) : X Y C: bilinear form Question. F Y, w X such that a(w, ϕ) = F (ϕ), ϕ Y with the estimate w X C F Y?

7 Assumption. (i) (bi-continuity) M > s.t. a(u, ϕ) M u X ϕ Y, u X, ϕ Y ; (ii) (decomposition by direct sum) N X {u X; a(u, ϕ) =, ϕ Y }, N Y {ϕ Y ; a(u, ϕ) =, u X} R X : closed subspace in X, R Y : closed subspace in Y s. t. X = N X R X (direct sum), Y = N Y R Y (direct sum). (iii) (variational inequality) C > s.t. u X C ϕ Y C ( sup ϕ Y ( sup u X a(u, ϕ) + P X u X ϕ Y a(u, ϕ) + P Y ϕ X u X ) ), u X,, ϕ Y, P X : X N X, P Y : Y N Y : projections.

8 Theorem. (generalization of the Lax-Milgram theorem) (X, X ): Banach space, (Y, Y ): reflexive Banach space a(, ) : X Y C: bilinear form satisfying the Assumption. F N Y, i.e., F Y with F (φ) =, φ N Y, w X such that with a(w, ϕ) = F (ϕ), w X C F Y, ϕ Y Remarks. (i) X need not be reflexive. (ii) Lax-Milgram theorem on the Hilbert space Theorem (iii) dim.n X <, dim.n Y < R X X, R Y Y : closed subspaces s. t. X = N X R X, Y = N Y R Y (direct sums). Theorem Fredholm alternative!

9 (iv) Fichera-Faedo s theorem W : normed space X, Y: Banach spaces S : W X, T : W Y: bounded linear operators k > s.t. T ϕ Y k Sϕ X, ϕ W F Y, g X s.t. g, Sϕ X,X = F, T ϕ Y,Y, ϕ W Lax-Milgarm theorem on the Hilbert space

10 3. Applications.; L r -de Rham-Hodge-Kodaira decomposition on Riemannian manifolds with the boundary. ( Ω, g): compact n-d Riemannian manifold with Ω C. ν T Ω τu = ν (ν u), νu = ν u for u l (T Ω), 1 l n, ν : l (T Ω) l 1 (T Ω): the interior product defined by (ν u)(x 1,, X l 1 ) = u(x 1,, X l 1, ν) for X 1,, X l 1 T Ω. u = τu + ν (νu) for all u l (T Ω). d : l (T Ω) l+1 (T Ω): the exterior derivative, l =, 1,, n 1, : l (T Ω) n l (T Ω): the Hodge star operator, l =, 1,, n, δ : l (T Ω) l 1 (T Ω): the co-differential operator, l = 1,, n, δ = ( 1) n+1 d χ n, χu = ( 1) l u for u l (T Ω) (u, v) Ω u v, for u, v l (T Ω).

11 E r d (Ω)l 1 {u L r (Ω) l 1 ; du L r (Ω) l }, E r δ (Ω)l {v L r (Ω) l ; δv L r (Ω) l 1 }, l = 1,, n, 1 < r < τ : u E r d (Ω)l 1 (Ω) τu W 1/r ( Ω) l 1 = (W 1 1/r,r ( Ω) l 1 ), ν : v E r δ (Ω)l νv W 1/r,r ( Ω) l 1 = (W 1 1/r,r ( Ω) l 1 ), s. t. the generalized Stokes integral formula holds: (du, v) (u, δv) = τu, νv Ω, l = 1,, n, {u, v} E r d (Ω)l 1 W 1,r (Ω) l or {u, v} W 1,r (Ω) l 1 E r δ (Ω)l. Xd r (Ω)l+1 {α W 1,r (Ω) l+1 ; dα = in Ω, να = on Ω}, Vδ r {β W 1,r (Ω) l 1 ; δβ = in Ω, τβ = on Ω}.

12 Theorem 3.1. ( Ω, g): compact n-dimensional Riemannian manifold, Ω C. 1 < r <, l = 1,, n 1. (i) ω L r (Ω) l, α X r d (Ω)l+1, β V r δ (Ω)l 1, h C (Ω) l L r (Ω) l with dh =, δh = s. t. with ω = δα + dβ + h α W 1,r + β W 1,r + h r C ω r. α X r d (Ω)l+1, β V r δ (Ω)l 1, h C (Ω) l L r (Ω) l with dh =, δh = s.t. ω = δα + dβ + h δα = δα, dβ = dβ, h = h. (ii) ω W s,r (Ω) l, s 1 α X r d (Ω)l+1 W s+1,r (Ω) l+1, β V r δ (Ω)l 1 W s+1,r (Ω) l 1, h C (Ω) W s,r (Ω) l with α W s+1,r + β W s+1,r + h W s,r C ω W s,r.

13 Corollary 3.2. (L r -Helmholtz-Weyl decomposition in 3D-domains) Ω R 3 : bounded domain, Ω C, 1 < r <. (i) u L r (Ω), α W 1,r (Ω) (scalar potential), β W 1,r (Ω): div β =, β ν Ω = (vector potential), h C ( Ω): div h =, rot h =, h ν Ω = (harmonic vector) s.t. u = α + rot β + h. (ii) u L r (Ω), β W 1,r (Ω), (scalar potential) α W 1,r (Ω) with div α =, α ν Ω = (vector potential), h C ( Ω) with div h =, rot h =, h ν Ω = (harmonic vector) s.t. u = β + rot α + h. Proof. Use Theorem 3.1 with g = (δ ij ) 1 i,j 3 the Euclidean metric. (i) n = 3, l = 2 (ii) n = 3, l = 1

14 Lemma 3.3. ( Ω, g):compact n-dimensional Riemannian manifold, Ω C. 1 < r <, l = 1,, n 1. (1) ω L r (Ω) l, α X r d (Ω)l+1 s.t. with (δα, δψ) = (ω, δψ), Ψ X r d (Ω)l+1 α W 1,r C ω r. ω W s,r (Ω) l, s 1 α X r d (Ω)l+1 W s+1,r (Ω) l+1 with (2) ω L r (Ω) l, β V r δ (Ω)l 1 s.t. with α W s+1,r C ω W s,r. (dβ, dψ) = (ω, dψ), ψ V r δ (Ω)l 1 β W 1,r C ω r. ω W s,r (Ω) l, s 1, β V r δ (Ω)l 1 W s+1,r (Ω) l 1 with β W s+1,r C ω W s,r.

15 Proof of Lemma 3.3. (1) X X r d (Ω)l+1, Y X r d (Ω)l+1, a(, ) : X Y C a(α, Ψ) (δα, δψ), α X, Ψ Y. u W s,r C( du W s 1,r + δu W s 1,r + u r + νu W s 1/r,r ( Ω) ), s 1 for u W s,r (Ω) l+1 (see e.g., Georgesgue) N X = {α X; a(α, Ψ) =, Ψ Y } N Y = {Ψ Y ; a(α, Ψ) =, α X} {H C ( Ω) l+1 ; dh =, δh = in Ω, νh = on Ω} X har (Ω) l+1 dim.x l+1 har (Ω) <. (Assumption (ii)) Variational inequality in X r d (Ω)l+1 α W 1,r C sup Ψ X r d (Ω)l+1 (δα, δψ) Ψ W 1,r + N i=1 (α, Ψ i ) for α X r d (Ω)l+1, where X har (Ω) l+1 = Span.{Ψ 1,, Ψ N }. (Assumption (iii)), 1 < r <

16 ω L r (Ω) l : given, Define F ω Y by F ω (Ψ) = (ω, δψ) for Ψ Y. F ω N Y, i.e., F ω(φ) =, Φ N Y = X har (Ω) l+1 & F ω Y ω r. Theorem α X r d (Ω)l+1 s.t. a(α, Ψ) = F ω (Ψ) (δα, δψ) = (ω, δψ), Ψ X r d (Ω)l+1. ω W s,r (Ω) l+1, s 1 α X r d (Ω)l+1 is characterized by the equations α = dω in Ω, dα = in Ω, να = on Ω. Agmon-Douglis-Nirenberg α X r d (Ω)l+1 W s+1,r (Ω) l+1. (2) The proof of (2) is similar to that of (1).

17 Assumption. (i) (bi-continuity) M > s.t. a(u, ϕ) M u X ϕ Y, u X, ϕ Y ; (ii) (decomposition of direct sums) N X {u X; a(u, ϕ) =, ϕ Y }, N Y {ϕ Y ; a(u, ϕ) =, u X} R X : closed subspace in X, R Y : closed subspace in Y s. t. X = N X R X (direct sum), Y = N Y R Y (direct sum). (iii) (variational inequalities) C > s.t. u X C ϕ Y C ( sup ϕ Y ( sup u X a(u, ϕ) + P X u X ϕ Y a(u, ϕ) + P Y ϕ X u X ) ), u X,, ϕ Y, P X : X N X, P Y : Y N Y : projections.

18 Theorem. (generalization of the Lax-Milgram theorem) (X, X ): Banach space, (Y, Y ): reflexive Banach space a(, ) : X Y C: bilinear form satisfying the Assumption. F N Y, i.e., F Y with F (φ) =, φ N Y, w X such that a(w, ϕ) = F (ϕ), ϕ Y with w X C F Y,

19 Proof of Theorem. decomposition (R X, X ), (R Y, Y ); Banach spaces T : R X R Y T w, ψ a(w, ψ), w R X, ψ R Y,, : duality pairing between R Y and R Y. bi-continuity T B(R X, R Y ) Claim 1. Range(T ) is closed in R Y. Use the variational inequality for a(, ) on X. Claim 2. Range(T ) = R Y Use Y = Y and the variational inequality for a(, ) on Y. f R Y, w R X s.t. T w = f, i.e., a(w, ψ) = f(ψ), ψ R Y.

20 Claim 3. F N Y, i.e., F Y, F (φ) =, φ N Y Indeed, a(w, ϕ) = F (ϕ), ϕ Y with w X C F Y. a(w, ϕ) = a(w, (1 P Y )ϕ) (P Y : Y N Y = {φ Y ; a(u, φ) =, u X}) = F ((1 P Y )ϕ) (Note that (1 P Y )ϕ R Y ) = F (ϕ) (Note that P Y ϕ N Y and F (P Y ϕ) = ) variational inequality for a(, ) on X w X C ( sup ϕ Y = C sup ϕ Y = C sup ϕ Y = C F Y ) a(w, ϕ) + P X w X ϕ Y a(w, ϕ) (Note that w R X P X w = ) ϕ Y F (ϕ) ϕ Y

21 Thank you for your attention!

New Helmholtz-Weyl decomposition in L r and its applications to the mathematical fluid mechanics

New Helmholtz-Weyl decomposition in L r and its applications to the mathematical fluid mechanics New Helmholtz-Weyl decomposition in L r and its applications to the mathematical fluid mechanics Hideo Kozono Mathematical Institute Tohoku University Sendai 980-8578 Japan Taku Yanagisawa Department of

More information

Theory of PDE Homework 2

Theory 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 information

Applied Math Qualifying Exam 11 October Instructions: Work 2 out of 3 problems in each of the 3 parts for a total of 6 problems.

Applied 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 information

Second Order Elliptic PDE

Second 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 information

Numerical Solutions to Partial Differential Equations

Numerical 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 information

LECTURE # 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) 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 information

Poincaré Duality Angles on Riemannian Manifolds with Boundary

Poincaré Duality Angles on Riemannian Manifolds with Boundary Poincaré Duality Angles on Riemannian Manifolds with Boundary Clayton Shonkwiler Department of Mathematics University of Pennsylvania June 5, 2009 Realizing cohomology groups as spaces of differential

More information

STOKES PROBLEM WITH SEVERAL TYPES OF BOUNDARY CONDITIONS IN AN EXTERIOR DOMAIN

STOKES PROBLEM WITH SEVERAL TYPES OF BOUNDARY CONDITIONS IN AN EXTERIOR DOMAIN Electronic Journal of Differential Equations, Vol. 2013 2013, No. 196, pp. 1 28. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu STOKES PROBLEM

More information

GEOMETRICAL TOOLS FOR PDES ON A SURFACE WITH ROTATING SHALLOW WATER EQUATIONS ON A SPHERE

GEOMETRICAL TOOLS FOR PDES ON A SURFACE WITH ROTATING SHALLOW WATER EQUATIONS ON A SPHERE GEOETRICAL TOOLS FOR PDES ON A SURFACE WITH ROTATING SHALLOW WATER EQUATIONS ON A SPHERE BIN CHENG Abstract. This is an excerpt from my paper with A. ahalov [1]. PDE theories with Riemannian geometry are

More information

Finite Elements. Colin Cotter. February 22, Colin Cotter FEM

Finite Elements. Colin Cotter. February 22, Colin Cotter FEM Finite Elements February 22, 2019 In the previous sections, we introduced the concept of finite element spaces, which contain certain functions defined on a domain. Finite element spaces are examples of

More information

WELL POSEDNESS OF PROBLEMS I

WELL POSEDNESS OF PROBLEMS I Finite Element Method 85 WELL POSEDNESS OF PROBLEMS I Consider the following generic problem Lu = f, where L : X Y, u X, f Y and X, Y are two Banach spaces We say that the above problem is well-posed (according

More information

THE LOCAL THEORY OF ELLIPTIC OPERATORS AND THE HODGE THEOREM

THE LOCAL THEORY OF ELLIPTIC OPERATORS AND THE HODGE THEOREM THE LOCAL THEORY OF ELLIPTIC OPERATORS AND THE HODGE THEOREM BEN LOWE Abstract. In this paper, we develop the local theory of elliptic operators with a mind to proving the Hodge Decomposition Theorem.

More information

[2] (a) Develop and describe the piecewise linear Galerkin finite element approximation of,

[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 information

From Completing the Squares and Orthogonal Projection to Finite Element Methods

From Completing the Squares and Orthogonal Projection to Finite Element Methods From Completing the Squares and Orthogonal Projection to Finite Element Methods Mo MU Background In scientific computing, it is important to start with an appropriate model in order to design effective

More information

P(E t, Ω)dt, (2) 4t has an advantage with respect. to the compactly supported mollifiers, i.e., the function W (t)f satisfies a semigroup law:

P(E t, Ω)dt, (2) 4t has an advantage with respect. to the compactly supported mollifiers, i.e., the function W (t)f satisfies a semigroup law: Introduction Functions of bounded variation, usually denoted by BV, have had and have an important role in several problems of calculus of variations. The main features that make BV functions suitable

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

Math212a Lecture 5 Applications of the spectral theorem for compact self-adjoint operators, 2. Gårding s inequality and its conseque

Math212a Lecture 5 Applications of the spectral theorem for compact self-adjoint operators, 2. Gårding s inequality and its conseque Math212a Lecture 5 Applications of the spectral theorem for compact self-adjoint operators, 2. Gårding s inequality and its consequences. September 16, 2014 1 Review of Sobolev spaces. Distributions and

More information

t y n (s) ds. t y(s) ds, x(t) = x(0) +

t 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 information

2.3 Variational form of boundary value problems

2.3 Variational form of boundary value problems 2.3. VARIATIONAL FORM OF BOUNDARY VALUE PROBLEMS 21 2.3 Variational form of boundary value problems Let X be a separable Hilbert space with an inner product (, ) and norm. We identify X with its dual X.

More information

HARMONIC FORMS ON NON-COMPACT RIEMANNIAN MANIFOLDS

HARMONIC FORMS ON NON-COMPACT RIEMANNIAN MANIFOLDS L 2 HARONIC FORS ON NON-COPACT RIEANNIAN ANIFOLDS GILLES CARRON First, I want to present some questions on L 2 - harmonic forms on non-compact Riemannian manifolds. Second, I will present an answer to

More information

INTRODUCTION TO PDEs

INTRODUCTION TO PDEs INTRODUCTION TO PDEs In this course we are interested in the numerical approximation of PDEs using finite difference methods (FDM). We will use some simple prototype boundary value problems (BVP) and initial

More information

The Dirichlet-to-Neumann operator

The Dirichlet-to-Neumann operator Lecture 8 The Dirichlet-to-Neumann operator The Dirichlet-to-Neumann operator plays an important role in the theory of inverse problems. In fact, from measurements of electrical currents at the surface

More information

Integral Representation Formula, Boundary Integral Operators and Calderón projection

Integral Representation Formula, Boundary Integral Operators and Calderón projection Integral Representation Formula, Boundary Integral Operators and Calderón projection Seminar BEM on Wave Scattering Franziska Weber ETH Zürich October 22, 2010 Outline Integral Representation Formula Newton

More information

On Friedrichs inequality, Helmholtz decomposition, vector potentials, and the div-curl lemma. Ben Schweizer 1

On Friedrichs inequality, Helmholtz decomposition, vector potentials, and the div-curl lemma. Ben Schweizer 1 On Friedrichs inequality, Helmholtz decomposition, vector potentials, and the div-curl lemma Ben Schweizer 1 January 16, 2017 Abstract: We study connections between four different types of results that

More information

Simple Examples on Rectangular Domains

Simple Examples on Rectangular Domains 84 Chapter 5 Simple Examples on Rectangular Domains In this chapter we consider simple elliptic boundary value problems in rectangular domains in R 2 or R 3 ; our prototype example is the Poisson equation

More information

Weak Formulation of Elliptic BVP s

Weak Formulation of Elliptic BVP s Weak Formulation of Elliptic BVP s There are a large number of problems of physical interest that can be formulated in the abstract setting in which the Lax-Milgram lemma is applied to an equation expressed

More information

Introduction to finite element exterior calculus

Introduction to finite element exterior calculus Introduction to finite element exterior calculus Ragnar Winther CMA, University of Oslo Norway Why finite element exterior calculus? Recall the de Rham complex on the form: R H 1 (Ω) grad H(curl, Ω) curl

More information

A very short introduction to the Finite Element Method

A very short introduction to the Finite Element Method A very short introduction to the Finite Element Method Till Mathis Wagner Technical University of Munich JASS 2004, St Petersburg May 4, 2004 1 Introduction This is a short introduction to the finite element

More information

Boundary-Value Problems for P.D.E.s

Boundary-Value Problems for P.D.E.s Boundary-Value Problems for P.D.E.s Contents:. P.D.E.s and boundary-value problems.. Elliptic equations in nondivergence form. 3. Green s formulae and related trace theorems. 4. The Fredholm alternative

More information

Chapter 1 Foundations of Elliptic Boundary Value Problems 1.1 Euler equations of variational problems

Chapter 1 Foundations of Elliptic Boundary Value Problems 1.1 Euler equations of variational problems Chapter 1 Foundations of Elliptic Boundary Value Problems 1.1 Euler equations of variational problems Elliptic boundary value problems often occur as the Euler equations of variational problems the latter

More information

Inequalities of Babuška-Aziz and Friedrichs-Velte for differential forms

Inequalities of Babuška-Aziz and Friedrichs-Velte for differential forms Inequalities of Babuška-Aziz and Friedrichs-Velte for differential forms Martin Costabel Abstract. For sufficiently smooth bounded plane domains, the equivalence between the inequalities of Babuška Aziz

More information

CS 468. Differential Geometry for Computer Science. Lecture 13 Tensors and Exterior Calculus

CS 468. Differential Geometry for Computer Science. Lecture 13 Tensors and Exterior Calculus CS 468 Differential Geometry for Computer Science Lecture 13 Tensors and Exterior Calculus Outline Linear and multilinear algebra with an inner product Tensor bundles over a surface Symmetric and alternating

More information

Konstantinos Chrysafinos 1 and L. Steven Hou Introduction

Konstantinos Chrysafinos 1 and L. Steven Hou Introduction Mathematical Modelling and Numerical Analysis Modélisation Mathématique et Analyse Numérique Will be set by the publisher ANALYSIS AND APPROXIMATIONS OF THE EVOLUTIONARY STOKES EQUATIONS WITH INHOMOGENEOUS

More information

Partial Differential Equations

Partial 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 information

NEGATIVE NORM SOBOLEV SPACES AND APPLICATIONS

NEGATIVE NORM SOBOLEV SPACES AND APPLICATIONS NEGATIVE NORM SOBOLEV SPACES AND APPLICATIONS MARCELO M. DISCONZI Abstract. We review the definition of negative Sobolev norms. As applications, we derive a necessary and sufficient condition for existence

More information

Complex manifolds, Kahler metrics, differential and harmonic forms

Complex manifolds, Kahler metrics, differential and harmonic forms Complex manifolds, Kahler metrics, differential and harmonic forms Cattani June 16, 2010 1 Lecture 1 Definition 1.1 (Complex Manifold). A complex manifold is a manifold with coordinates holomorphic on

More information

The Factorization Method for Inverse Scattering Problems Part I

The Factorization Method for Inverse Scattering Problems Part I The Factorization Method for Inverse Scattering Problems Part I Andreas Kirsch Madrid 2011 Department of Mathematics KIT University of the State of Baden-Württemberg and National Large-scale Research Center

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

TD 1: Hilbert Spaces and Applications

TD 1: Hilbert Spaces and Applications Université Paris-Dauphine Functional Analysis and PDEs Master MMD-MA 2017/2018 Generalities TD 1: Hilbert Spaces and Applications Exercise 1 (Generalized Parallelogram law). Let (H,, ) be a Hilbert space.

More information

Non-stationary Friedrichs systems

Non-stationary Friedrichs systems Department of Mathematics, University of Osijek BCAM, Bilbao, November 2013 Joint work with Marko Erceg 1 Stationary Friedrichs systems Classical theory Abstract theory 2 3 Motivation Stationary Friedrichs

More information

MATH 263: PROBLEM SET 1: BUNDLES, SHEAVES AND HODGE THEORY

MATH 263: PROBLEM SET 1: BUNDLES, SHEAVES AND HODGE THEORY MATH 263: PROBLEM SET 1: BUNDLES, SHEAVES AND HODGE THEORY 0.1. Vector Bundles and Connection 1-forms. Let E X be a complex vector bundle of rank r over a smooth manifold. Recall the following abstract

More information

INF-SUP CONDITION FOR OPERATOR EQUATIONS

INF-SUP CONDITION FOR OPERATOR EQUATIONS INF-SUP CONDITION FOR OPERATOR EQUATIONS LONG CHEN We study the well-posedness of the operator equation (1) T u = f. where T is a linear and bounded operator between two linear vector spaces. We give equivalent

More information

Geometric PDE and The Magic of Maximum Principles. Alexandrov s Theorem

Geometric 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 information

Contents: 1. Minimization. 2. The theorem of Lions-Stampacchia for variational inequalities. 3. Γ -Convergence. 4. Duality mapping.

Contents: 1. Minimization. 2. The theorem of Lions-Stampacchia for variational inequalities. 3. Γ -Convergence. 4. Duality mapping. Minimization Contents: 1. Minimization. 2. The theorem of Lions-Stampacchia for variational inequalities. 3. Γ -Convergence. 4. Duality mapping. 1 Minimization A Topological Result. Let S be a topological

More information

Least-Squares Finite Element Methods

Least-Squares Finite Element Methods Pavel В. Bochev Max D. Gunzburger Least-Squares Finite Element Methods Spri ringer Contents Part I Survey of Variational Principles and Associated Finite Element Methods 1 Classical Variational Methods

More information

Variational Formulations

Variational Formulations Chapter 2 Variational Formulations In this chapter we will derive a variational (or weak) formulation of the elliptic boundary value problem (1.4). We will discuss all fundamental theoretical results that

More information

SPECTRAL PROPERTIES OF THE LAPLACIAN ON BOUNDED DOMAINS

SPECTRAL PROPERTIES OF THE LAPLACIAN ON BOUNDED DOMAINS SPECTRAL PROPERTIES OF THE LAPLACIAN ON BOUNDED DOMAINS TSOGTGEREL GANTUMUR Abstract. After establishing discrete spectra for a large class of elliptic operators, we present some fundamental spectral properties

More information

RIEMANN-HILBERT PROBLEM FOR THE MOISIL-TEODORESCU SYSTEM IN MULTIPLE CONNECTED DOMAINS

RIEMANN-HILBERT PROBLEM FOR THE MOISIL-TEODORESCU SYSTEM IN MULTIPLE CONNECTED DOMAINS Electronic Journal of Differential Equations, Vol. 2016 (2016), No. 310, pp. 1 5. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu RIEMANN-HILBERT PROBLEM FOR THE MOISIL-TEODORESCU

More information

Existence, stability and instability for Einstein-scalar field Lichnerowicz equations by Emmanuel Hebey

Existence, stability and instability for Einstein-scalar field Lichnerowicz equations by Emmanuel Hebey Existence, stability and instability for Einstein-scalar field Lichnerowicz equations by Emmanuel Hebey Joint works with Olivier Druet and with Frank Pacard and Dan Pollack Two hours lectures IAS, October

More information

Lecture 4: Harmonic forms

Lecture 4: Harmonic forms Lecture 4: Harmonic forms Jonathan Evans 29th September 2010 Jonathan Evans () Lecture 4: Harmonic forms 29th September 2010 1 / 15 Jonathan Evans () Lecture 4: Harmonic forms 29th September 2010 2 / 15

More information

Cohomology of Harmonic Forms on Riemannian Manifolds With Boundary

Cohomology of Harmonic Forms on Riemannian Manifolds With Boundary Cohomology of Harmonic Forms on Riemannian Manifolds With Boundary Sylvain Cappell, Dennis DeTurck, Herman Gluck, and Edward Y. Miller 1. Introduction To Julius Shaneson on the occasion of his 60th birthday

More information

Your first day at work MATH 806 (Fall 2015)

Your first day at work MATH 806 (Fall 2015) Your first day at work MATH 806 (Fall 2015) 1. Let X be a set (with no particular algebraic structure). A function d : X X R is called a metric on X (and then X is called a metric space) when d satisfies

More information

FINITE ENERGY SOLUTIONS OF MIXED 3D DIV-CURL SYSTEMS

FINITE ENERGY SOLUTIONS OF MIXED 3D DIV-CURL SYSTEMS FINITE ENERGY SOLUTIONS OF MIXED 3D DIV-CURL SYSTEMS GILES AUCHMUTY AND JAMES C. ALEXANDER Abstract. This paper describes the existence and representation of certain finite energy (L 2 -) solutions of

More information

Navier-Stokes equations in thin domains with Navier friction boundary conditions

Navier-Stokes equations in thin domains with Navier friction boundary conditions Navier-Stokes equations in thin domains with Navier friction boundary conditions Luan Thach Hoang Department of Mathematics and Statistics, Texas Tech University www.math.umn.edu/ lhoang/ luan.hoang@ttu.edu

More information

Some Notes on Elliptic Regularity

Some Notes on Elliptic Regularity Some Notes on Elliptic Regularity Here we consider first the existence of weak solutions to elliptic problems of the form: { Lu = f, u = 0, (1) and then we consider the regularity of such solutions. The

More information

Divergence Boundary Conditions for Vector Helmholtz Equations with Divergence Constraints

Divergence Boundary Conditions for Vector Helmholtz Equations with Divergence Constraints Divergence Boundary Conditions for Vector Helmholtz Equations with Divergence Constraints Urve Kangro Department of Mathematical Sciences Carnegie Mellon University Pittsburgh, PA 15213 Roy Nicolaides

More information

Lecture Notes on PDEs

Lecture Notes on PDEs Lecture Notes on PDEs Alberto Bressan February 26, 2012 1 Elliptic equations Let IR n be a bounded open set Given measurable functions a ij, b i, c : IR, consider the linear, second order differential

More information

and finally, any second order divergence form elliptic operator

and finally, any second order divergence form elliptic operator Supporting Information: Mathematical proofs Preliminaries Let be an arbitrary bounded open set in R n and let L be any elliptic differential operator associated to a symmetric positive bilinear form B

More information

Section 2. Basic formulas and identities in Riemannian geometry

Section 2. Basic formulas and identities in Riemannian geometry Section 2. Basic formulas and identities in Riemannian geometry Weimin Sheng and 1. Bianchi identities The first and second Bianchi identities are R ijkl + R iklj + R iljk = 0 R ijkl,m + R ijlm,k + R ijmk,l

More information

Regularity Theory a Fourth Order PDE with Delta Right Hand Side

Regularity Theory a Fourth Order PDE with Delta Right Hand Side Regularity Theory a Fourth Order PDE with Delta Right Hand Side Graham Hobbs Applied PDEs Seminar, 29th October 2013 Contents Problem and Weak Formulation Example - The Biharmonic Problem Regularity Theory

More information

Geometry and the Kato square root problem

Geometry and the Kato square root problem Geometry and the Kato square root problem Lashi Bandara Centre for Mathematics and its Applications Australian National University 7 June 2013 Geometric Analysis Seminar University of Wollongong Lashi

More information

Inverse Scattering with Partial data on Asymptotically Hyperbolic Manifolds

Inverse Scattering with Partial data on Asymptotically Hyperbolic Manifolds Inverse Scattering with Partial data on Asymptotically Hyperbolic Manifolds Raphael Hora UFSC rhora@mtm.ufsc.br 29/04/2014 Raphael Hora (UFSC) Inverse Scattering with Partial data on AH Manifolds 29/04/2014

More information

New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space

New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space Chérif Amrouche, Huy Hoang Nguyen To cite this version: Chérif Amrouche, Huy Hoang Nguyen. New estimates

More information

On positive solutions of semi-linear elliptic inequalities on Riemannian manifolds

On positive solutions of semi-linear elliptic inequalities on Riemannian manifolds On positive solutions of semi-linear elliptic inequalities on Riemannian manifolds Alexander Grigor yan University of Bielefeld University of Minnesota, February 2018 Setup and problem statement Let (M,

More information

LECTURE 1: SOURCES OF ERRORS MATHEMATICAL TOOLS A PRIORI ERROR ESTIMATES. Sergey Korotov,

LECTURE 1: SOURCES OF ERRORS MATHEMATICAL TOOLS A PRIORI ERROR ESTIMATES. Sergey Korotov, LECTURE 1: SOURCES OF ERRORS MATHEMATICAL TOOLS A PRIORI ERROR ESTIMATES Sergey Korotov, Institute of Mathematics Helsinki University of Technology, Finland Academy of Finland 1 Main Problem in Mathematical

More information

THE HODGE DECOMPOSITION

THE HODGE DECOMPOSITION THE HODGE DECOMPOSITION KELLER VANDEBOGERT 1. The Musical Isomorphisms and induced metrics Given a smooth Riemannian manifold (X, g), T X will denote the tangent bundle; T X the cotangent bundle. The additional

More information

Finite difference method for elliptic problems: I

Finite 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 information

CS 468 (Spring 2013) Discrete Differential Geometry

CS 468 (Spring 2013) Discrete Differential Geometry CS 468 (Spring 2013) Discrete Differential Geometry Lecture 13 13 May 2013 Tensors and Exterior Calculus Lecturer: Adrian Butscher Scribe: Cassidy Saenz 1 Vectors, Dual Vectors and Tensors 1.1 Inner Product

More information

The Helmholtz Equation

The Helmholtz Equation The Helmholtz Equation Seminar BEM on Wave Scattering Rene Rühr ETH Zürich October 28, 2010 Outline Steklov-Poincare Operator Helmholtz Equation: From the Wave equation to Radiation condition Uniqueness

More information

A study of some curvature operators near the Euclidian metric

A study of some curvature operators near the Euclidian metric A study of some curvature operators near the Euclidian metric Erwann Delay Univ. Avignon Jussieu, 28 mai 2014 A geometric operator Let κ, Λ R and let Ein(g) = Ric(g) + κr(g) g + Λ g S 2. Φ (Ein(g)) = Ein(Φ

More information

Scientific Computing WS 2018/2019. Lecture 15. Jürgen Fuhrmann Lecture 15 Slide 1

Scientific Computing WS 2018/2019. Lecture 15. Jürgen Fuhrmann Lecture 15 Slide 1 Scientific Computing WS 2018/2019 Lecture 15 Jürgen Fuhrmann juergen.fuhrmann@wias-berlin.de Lecture 15 Slide 1 Lecture 15 Slide 2 Problems with strong formulation Writing the PDE with divergence and gradient

More information

A Note on the Variational Formulation of PDEs and Solution by Finite Elements

A Note on the Variational Formulation of PDEs and Solution by Finite Elements Advanced Studies in Theoretical Physics Vol. 12, 2018, no. 4, 173-179 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/astp.2018.8412 A Note on the Variational Formulation of PDEs and Solution by

More information

LORENTZ SPACE ESTIMATES FOR VECTOR FIELDS WITH DIVERGENCE AND CURL IN HARDY SPACES

LORENTZ SPACE ESTIMATES FOR VECTOR FIELDS WITH DIVERGENCE AND CURL IN HARDY SPACES - TAMKANG JOURNAL OF MATHEMATICS Volume 47, Number 2, 249-260, June 2016 doi:10.5556/j.tkjm.47.2016.1932 This paper is available online at http://journals.math.tku.edu.tw/index.php/tkjm/pages/view/onlinefirst

More information

Finite Element Exterior Calculus and Applications Part V

Finite Element Exterior Calculus and Applications Part V Finite Element Exterior Calculus and Applications Part V Douglas N. Arnold, University of Minnesota Peking University/BICMR August 15 18, 2015 De Rham complex 0 H 1 (Ω) grad H(curl, Ω) curl H(div, Ω) div

More information

MINIMAL 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 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 information

Geometry and the Kato square root problem

Geometry and the Kato square root problem Geometry and the Kato square root problem Lashi Bandara Centre for Mathematics and its Applications Australian National University 7 June 2013 Geometric Analysis Seminar University of Wollongong Lashi

More information

Boundary regularity of solutions of degenerate elliptic equations without boundary conditions

Boundary regularity of solutions of degenerate elliptic equations without boundary conditions Boundary regularity of solutions of elliptic without boundary Iowa State University November 15, 2011 1 2 3 4 If the linear second order elliptic operator L is non with smooth coefficients, then, for any

More information

A Concise Course on Stochastic Partial Differential Equations

A Concise Course on Stochastic Partial Differential Equations A Concise Course on Stochastic Partial Differential Equations Michael Röckner Reference: C. Prevot, M. Röckner: Springer LN in Math. 1905, Berlin (2007) And see the references therein for the original

More information

Appendix A Functional Analysis

Appendix A Functional Analysis Appendix A Functional Analysis A.1 Metric Spaces, Banach Spaces, and Hilbert Spaces Definition A.1. Metric space. Let X be a set. A map d : X X R is called metric on X if for all x,y,z X it is i) d(x,y)

More information

Introduction to Index Theory. Elmar Schrohe Institut für Analysis

Introduction to Index Theory. Elmar Schrohe Institut für Analysis Introduction to Index Theory Elmar Schrohe Institut für Analysis Basics Background In analysis and pde, you want to solve equations. In good cases: Linearize, end up with Au = f, where A L(E, F ) is a

More information

Fredholm Theory. April 25, 2018

Fredholm Theory. April 25, 2018 Fredholm Theory April 25, 208 Roughly speaking, Fredholm theory consists of the study of operators of the form I + A where A is compact. From this point on, we will also refer to I + A as Fredholm operators.

More information

Extension and Representation of Divergence-free Vector Fields on Bounded Domains. Tosio Kato, Marius Mitrea, Gustavo Ponce, and Michael Taylor

Extension and Representation of Divergence-free Vector Fields on Bounded Domains. Tosio Kato, Marius Mitrea, Gustavo Ponce, and Michael Taylor Extension and Representation of Divergence-free Vector Fields on Bounded Domains Tosio Kato, Marius Mitrea, Gustavo Ponce, and Michael Taylor 1. Introduction Let Ω R n be a bounded, connected domain, with

More information

Weierstraß-Institut. für Angewandte Analysis und Stochastik. Leibniz-Institut im Forschungsverbund Berlin e. V. Preprint ISSN

Weierstraß-Institut. für Angewandte Analysis und Stochastik. Leibniz-Institut im Forschungsverbund Berlin e. V. Preprint ISSN Weierstraß-Institut für Angewandte Analysis und Stochastik Leibniz-Institut im Forschungsverbund Berlin e. V. Preprint ISSN 2198-5855 On the divergence constraint in mixed finite element methods for incompressible

More information

Mathematical analysis of the stationary Navier-Stokes equations

Mathematical analysis of the stationary Navier-Stokes equations Mathematical analysis of the Department of Mathematics, Sogang University, Republic of Korea The 3rd GCOE International Symposium Weaving Science Web beyond Particle Matter Hierarchy February 17-19, 2011,

More information

On the bang-bang property of time optimal controls for infinite dimensional linear systems

On the bang-bang property of time optimal controls for infinite dimensional linear systems On the bang-bang property of time optimal controls for infinite dimensional linear systems Marius Tucsnak Université de Lorraine Paris, 6 janvier 2012 Notation and problem statement (I) Notation: X (the

More information

L p estimates for parabolic equations in Reifenberg domains

L 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 information

Elliptic Partial Differential Equations of Second Order

Elliptic Partial Differential Equations of Second Order David Gilbarg Neil S.Trudinger Elliptic Partial Differential Equations of Second Order Reprint of the 1998 Edition Springer Chapter 1. Introduction 1 Part I. Linear Equations Chapter 2. Laplace's Equation

More information

The heat equation in time dependent domains with Neumann boundary conditions

The heat equation in time dependent domains with Neumann boundary conditions The heat equation in time dependent domains with Neumann boundary conditions Chris Burdzy Zhen-Qing Chen John Sylvester Abstract We study the heat equation in domains in R n with insulated fast moving

More information

The Navier-Stokes problem in velocity-pressure formulation :convergence and Optimal Control

The 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 information

RIEMANN S INEQUALITY AND RIEMANN-ROCH

RIEMANN S INEQUALITY AND RIEMANN-ROCH RIEMANN S INEQUALITY AND RIEMANN-ROCH DONU ARAPURA Fix a compact connected Riemann surface X of genus g. Riemann s inequality gives a sufficient condition to construct meromorphic functions with prescribed

More information

Tutorial 2. Introduction to numerical schemes

Tutorial 2. Introduction to numerical schemes 236861 Numerical Geometry of Images Tutorial 2 Introduction to numerical schemes c 2012 Classifying PDEs Looking at the PDE Au xx + 2Bu xy + Cu yy + Du x + Eu y + Fu +.. = 0, and its discriminant, B 2

More information

MEYERS TYPE ESTIMATES FOR APPROXIMATE SOLUTIONS OF NONLINEAR ELLIPTIC EQUATIONS AND THEIR APPLICATIONS. Yalchin Efendiev.

MEYERS TYPE ESTIMATES FOR APPROXIMATE SOLUTIONS OF NONLINEAR ELLIPTIC EQUATIONS AND THEIR APPLICATIONS. Yalchin Efendiev. Manuscript submitted to AIMS Journals Volume X, Number 0X, XX 200X Website: http://aimsciences.org pp. X XX MEYERS TYPE ESTIMATES FOR APPROXIMATE SOLUTIONS OF NONLINEAR ELLIPTIC EUATIONS AND THEIR APPLICATIONS

More information

Traces, extensions and co-normal derivatives for elliptic systems on Lipschitz domains

Traces, extensions and co-normal derivatives for elliptic systems on Lipschitz domains Traces, extensions and co-normal derivatives for elliptic systems on Lipschitz domains Sergey E. Mikhailov Brunel University West London, Department of Mathematics, Uxbridge, UB8 3PH, UK J. Math. Analysis

More information

ON WEAKLY NONLINEAR BACKWARD PARABOLIC PROBLEM

ON WEAKLY NONLINEAR BACKWARD PARABOLIC PROBLEM ON WEAKLY NONLINEAR BACKWARD PARABOLIC PROBLEM OLEG ZUBELEVICH DEPARTMENT OF MATHEMATICS THE BUDGET AND TREASURY ACADEMY OF THE MINISTRY OF FINANCE OF THE RUSSIAN FEDERATION 7, ZLATOUSTINSKY MALIY PER.,

More information

Introduction to numerical schemes

Introduction to numerical schemes 236861 Numerical Geometry of Images Tutorial 2 Introduction to numerical schemes Heat equation The simple parabolic PDE with the initial values u t = K 2 u 2 x u(0, x) = u 0 (x) and some boundary conditions

More information

On the p-laplacian and p-fluids

On the p-laplacian and p-fluids LMU Munich, Germany Lars Diening On the p-laplacian and p-fluids Lars Diening On the p-laplacian and p-fluids 1/50 p-laplacian Part I p-laplace and basic properties Lars Diening On the p-laplacian and

More information

CONVERGENCE THEORY. G. ALLAIRE CMAP, Ecole Polytechnique. 1. Maximum principle. 2. Oscillating test function. 3. Two-scale convergence

CONVERGENCE THEORY. G. ALLAIRE CMAP, Ecole Polytechnique. 1. Maximum principle. 2. Oscillating test function. 3. Two-scale convergence 1 CONVERGENCE THEOR G. ALLAIRE CMAP, Ecole Polytechnique 1. Maximum principle 2. Oscillating test function 3. Two-scale convergence 4. Application to homogenization 5. General theory H-convergence) 6.

More information

9. Boundary value problems in a constant-coefficient case

9. Boundary value problems in a constant-coefficient case 9.1 9. Boundary value problems in a constant-coefficient case 9.1. Boundary maps for the half-space. We have considered various realizations in Section 4.4 of the Laplacian and similar operators, defined

More information

A Finite Element Method for the Surface Stokes Problem

A Finite Element Method for the Surface Stokes Problem J A N U A R Y 2 0 1 8 P R E P R I N T 4 7 5 A Finite Element Method for the Surface Stokes Problem Maxim A. Olshanskii *, Annalisa Quaini, Arnold Reusken and Vladimir Yushutin Institut für Geometrie und

More information

Gradient estimates for eigenfunctions on compact Riemannian manifolds with boundary

Gradient 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 information