REGULARITY OF SOLUTIONS OF PARTIAL NEUTRAL FUNCTIONAL DIFFERENTIAL EQUATIONS WITH UNBOUNDED DELAY

Size: px
Start display at page:

Download "REGULARITY OF SOLUTIONS OF PARTIAL NEUTRAL FUNCTIONAL DIFFERENTIAL EQUATIONS WITH UNBOUNDED DELAY"

Transcription

1 Proyecciones Vol. 21, N o 1, pp , May 22. Universidad Católica del Norte Antofagasta - Cile REGULARITY OF SOLUTIONS OF PARTIAL NEUTRAL FUNCTIONAL DIFFERENTIAL EQUATIONS WITH UNBOUNDED DELAY EDUARDO HERNÁNDEZ Universidade de Sao Paulo - Brasil Abstract We prove te existence of regular solutions for a class of quasi-linear partial neutral functional differential equations wit unbounded delay tat can be described as te abstract retarded functional differential equation d dt (x(t) + F (t, x t)) = Ax(t) + G(t, x t ), were A is te infinitesimal generator of a strongly continuous semigroup of bounded linear operators on a Banac space X and F, G are appropriated functions. Keywords: Retarded functional differential equations, abstract Caucy problem, semigroup of bounded linear operators, regularity of solutions. Researc Partially Supported by FAPESP-SP-Brazil, grant #

2 66 Eduardo Hernández 1. Introduction Te purpose of tis paper is to establis some results of regularity, in a sense to be specified later, for solutions of a class of quasi-linear neutral functional differential equations wit unbounded delay tat can be described in te form (1.1) { d dt (x(t) + F (t, x t)) = Ax(t) + G(t, x t ), t > σ, x σ = ϕ B, were A is te infinitesimal generator of an uniformly bounded analytic semigroup of bounded linear operators, (T (t)) t, on a Banac space X, te istory x t : (, ] X, x t (θ) = x(t + θ), belongs to some abstract pase space B defined axiomatically, Ω B is open, σ < a and F, G : [σ, a] Ω X are appropriate continuous functions. Neutral differential equations arise in many areas of applied matematics and suc equations ave received muc attention in recent years. A good guide to te literature for neutral functional differential equations is te Hale & lunel book [3] and te references terein. Te work in partial neutral functional differential equations wit unbounded delay was initiated by Hernández & Henríquez in [4, 5]. In tese papers, Hernández & Henríquez proved te existence of mild, strong and periodic solutions for te neutral equation (1.1). In general, te results were obtained using te semigroup teory and te Sadovskii fixed point teorem ( see [11] ). Te results obtained in tis paper are te continuation of papers [4], [5] on te existence of mild, strong and periodical solutions for te neutral system (1.1) and generalization of te results reported by Henriquez in [6]. Trougout tis paper, X will be a Banac space provided wit norm and A : D(A) X will be te infinitesimal generator of an uniformly bounded analytic semigroup, T = (T (t)) t, of linear operators on X. For te teory of strongly continuous semigroup, we refer to Pazy [1] and Krein [9]. We will point out ere some notations and properties tat will be used in tis work. It is well know tat tere exist constants M and w IR suc tat T (t) Me wt, t.

3 Regularity of Solutions of Partial Neutral Functional 67 If T is a uniformly bounded and analytic semigroup suc tat ρ(a), ten it is possible to define te fractional power ( A) α, for < α 1, as a closed linear operator on its domain D( A) α. Furtermore, te subspace D( A) α is dense in X, and te expression x α = ( A) α x defines a norm in D( A) α. If X α represents te space D( A) α endowed wit te norm α, ten te following properties are well known ([1], pp. 74 ): Lemma 1. If te previous conditions old: 1. Let < α 1. Ten X α is a Banac space. 2. If < β α ten X α X β is continuous. 3. For every constant a >, tere exists C a > suc tat ( A) α T (t) C a t α, < t a. 4. For every a > tere exists a positive constant C a suc tat (T (t) I)( A) α C a t α, < t a. In tis work we will employ an axiomatic definition of te pase space B, introduced by Hale and Kato [2]. To establis te axioms of te space B we follows te terminology used in Hino-Murakami-Naito [8], and tus, B will be a linear space of functions mapping (, ] into X, endowed wit a seminorm B. We will assume tat B satisfies te following axioms: (A) If x : (, σ +ω) X, ω >, is continuous on [σ, σ +ω) and x σ B, ten for every t [σ, σ + ω) te following conditions old: i) x t is in B. ii) x(t) H x t B.

4 68 Eduardo Hernández iii) x t B K(t σ) sup{ x(s) : σ s t} + M(t σ) x σ B. Were H > is a constant; K, M : [, ) [, ), K is continuous, M is locally bounded and H, K, M are independent of x ( ). (A 1) For te function x ( ) in (A), x t is a B-.valued continuous function on [σ, σ + w). (B) Te space B is complete. For te literature on pase space, we refer te reader to [8]. Wile noting ere tat from te axiom (A 1), it follows, tat te operator function W ( ) dfined by (1.2)[W (t) ϕ] (θ) := { T (t + θ) ϕ () for t θ, ϕ (t + θ) for < θ < t, is an strongly continuous semigroup of bounded linear operators on B. In tis paper, A w wit domain D (A w ) will be te infinitesimal generator of W ( ). To obtain some of our results we will require additional properties for te pase space B, in particular we consider te following axiom (see [6], pp. 526 for details) ; (C 3 ) Let ρ >. Let x : (, σ + ρ] X be a continuous function suc tat x σ and te rigt derivative, denoted x (σ + ), exists. If te function ψ defined by ψ (θ) = for θ < and ψ () := x (σ + ) belongs to B ten ( 1 ) xσ+ ψ B as +. On te oter and, for a linear map P : D (P ) X X and ϕ B suc tat ϕ (θ) D (P ) for every θ, we denote by P ϕ : (, ] X, defined by P ϕ = P (ϕ(θ)). For any < α 1 we use te notation B α for te vector space B α = {( A) α ϕ : ϕ B }. It is easily to prove tat B α, endowed wit te seminorm defined by ψ Bα := ( A) α ψ B,

5 Regularity of Solutions of Partial Neutral Functional 69 is a pase space of functions wit values in X α. Te paper is organized as follows. In section 2, we define te different concepts used in tis work and establis te existence of N-classical and classical solutions for te initial value problem (1.1). Our results are based on te properties of analytic semigroups and te ideas contained in Pazy [1] and Henríquez [6]. Trougout tis work we assume tat X is an abstract Banac space. Te terminology and notations are tose generally used in operator teory. In particular, if X and Y are Banac spaces, we indicate by L (X : Y ) te Banac space of te bounded linear operators of X in Y and we abbreviate tis notation to L (X) wen ever X = Y. In addition B r (x : X) will denote te closed ball in te space X wit center at x and radius r. For some bounded function ξ : [σ, a] X and σ s < t a we employ te notation (1.3) ξ( ) [s,t] = sup{ ξ(θ) : θ [s, t]} and we will write simply ξ t for ξ( ) [σ,t] wen no confusion arises. If x X, we will use te notation X x for te function X x : (, ] X were X x = for θ < and X x () = x. Finally, a function f : I IR X is α-hölder continuous, < α 1, if tere exists a constant L > suc tat f(s) f(t) L t s α, s, t I. We represent by C, α (I; X) te space of α-hölder continuous function from I into X. Similarly, C k, α (I; X) consist of tose functions from I into X, tat are k-times continuously differentiable and wose k t -derivative is α-hölder continuous.

6 7 Eduardo Hernández 2. Regularity of Mild Solutions In tis section we will study te regularity of mild solutions of te abstract Caucy problem (1.1). Hencefort we will assume tat A is te infinitesimal generator of a uniformly bounded analytic semigroup, T = (T (t)) t, on X, tat Ω B is open and tat F, G : [σ, a] Ω X are continuous functions. Furter, to avoid unnecessary notation, we suppose tat ρ(a) and tat T (t) M, for some constant M 1 and every t. Our regularity results are based on tose of regularity of mild solutions for te abstract Caucy problem (2.1) { x (t) = Ax(t) + f(t), x() = x. By analogy wit te abstract Caucy problem (2.1) we adopt te following definitions: Definition 1. We will say tat a function x : (, σ +b) X, σ + b a, is a mild solution of te abstract Caucy problem (1.1) if: x σ = ϕ; te restriction of x( ) to te interval [σ, σ + b) is continuous; for eac σ t < σ+b te function AT (t s)f (s, x s ), s [σ, t), is integrable and (2.2) x(t) = T (t σ)(ϕ() + F (σ, ϕ)) F (t, x t ) t σ AT (t s)f (s, x s)ds + t σ T (t s)g(s, x s)ds, for every t [σ, σ + b). Te existence and uniqueness of mild solution of system (1.1) was establised in [5] as consequence of te contraction principle. More precisely: Teorem 1. Let ϕ Ω and assume tat te following conditions old: a) Tere exist β (, 1) and L suc tat te function F is X β -valued and satisfies te Lipscitz condition ( A) β F (t, ψ 1 ) ( A) β F (s, ψ 2 ) (2.3) L ( t s + ψ 1 ψ 2 B )

7 Regularity of Solutions of Partial Neutral Functional 71 for every σ s, t a, ψ 1, ψ 2 Ω and (2.4) K()L ( A) β < 1. b) Te function G is continuous and tere exist N > suc tat G(t, ψ 1 ) G(s, ψ 2 ) (2.5) N( t s + ψ 1 ψ 2 B ) for every σ s, t a and ψ 1, ψ 2 Ω. Ten tere exists a unique mild solution x(, ϕ) of te abstract Caucy problem (1.1) defined on (, σ + r), for some < r < a σ. Furtermore, if Ω = B ten r can be cosen independent of ϕ. Considering te concepts of mild and classical solutions adopted by Henriquez in [6], we introduce te followings definitions. Definition 2. We will say tat a function x : (, σ +b) X, b >, is a classical solution of te abstract Caucy problem (1.1) if: x σ = ϕ; x( ) C([σ, σ + b); X) C 1 ((σ, σ + b); X); x(t) D(A) for every t (σ, σ + b); for eac σ t < σ + b te function AT (t s)f (s, x s ), s [σ, t), is integrable and x( ) satisfies equation (1.1) on [σ, σ + b). Definition 3. We will say tat a function x : (, σ +b) X, b >, is an N-classical solution of te abstract Caucy problem (1.1) if: x σ = ϕ, x( ) C([σ, σ + b); X); x(t) D(A) for every d t (σ, σ + b); dt (x(t) + F (t, x t)) is continuous on (σ, σ + b); for eac σ t < σ + b te function AT (t s)f (s, x s ), s [σ, t), is integrable and x( ) satisfies equation (1.1) on [σ, σ + b). In relation wit te previous definitions, we consider te following result. Proposition 1. Te following properties old.

8 72 Eduardo Hernández (a) If x( ) : (, σ+b) X is a classical or N-classical solution of (1.1) ten x( ) is a mild solution. (b) If x( ) : (, σ + b) X is a N-classical solution of (1.1) and d dt F (t, x t) is continuous on (σ, σ + b), ten x( ) is a classical solution. (c) Every classical solution is a N-classical solution. Proof: We only prove (a). Using tat (T (t)) t is analytic; for t, s [σ, σ + b) wit t > s, we find tat d [T (t s)(x(s) + F (s, x ds s))] = AT (t s)(x(s) + F (s, x s )) +T (t s) d (x(s) + F (s, x ds s)) = AT (t s)f (s, x s + T (t s)g(s, x s ), wic in turn implies tat x(t) + F (t, x t ) = T (t σ)(ϕ() + F (σ, ϕ)) t σ AT (t s)f (s, x s)ds + t σ T (t s)g(s, x s)ds, since s AT (t s)f (s, x s ) is integrable on [σ, t). Tus x( ) is a mild solution. Te proof is complete To prove our first regularity Teorem, we need previously some tecnical results. Next, we study te regularity of mild solutions of te abstract Caucy problem ẋ(t) = Ax(t) + ( A) 1 β g(t), (2.6) x() =, were g( ) C([, a]; X 1 β ) C, ϑ ([, a]; X); β, ϑ (, 1) and β + ϑ > 1. To tis end, for a mild solution, u( ), of (2.6) we introduce te decomposition u (t) = t ( A)1 β T (t s)(g(s) g(t))ds + t ( A)1 β T (t s)g(t)ds = u 1 (t) + u 2 (t).

9 Regularity of Solutions of Partial Neutral Functional 73 Te proofs of te following tree results follow from te proofs of Teorems 4.3.2, and Lemma in Pazy [1]. However tere are some differences tat require special attention and we include te principal ideas of te proofs for completeness. Lemma 2. Let ϑ, β (, 1) wit β + ϑ > 1 and g( ) C([, a]; X 1 β ) C, ϑ ([, a]; X). If u( ) is a mild solution of (2.6) ten u( ) C([, a]; X 1 ) C 1 ([, a]; X). Proof. Clearly Au 2 (t) C ([, a] ; X), since Au 2 (t) = T ( A) 1 β g (t) ( A) 1 β g (t). In order to study te function u 1, for ɛ > we define te function u 1,ɛ C ([, a] ; X) by u 1,ɛ (t) := (2.7) t ɛ ( A) 1 β T (t s) (g (s) g (t)) ds, for t [ɛ, a], for t [, ɛ), From Lemma in [1], u 1,ɛ (t) D(A) for every t [, a] and Au 1,ɛ (t) := (2.8) { t ɛ ( A) 2 β T (t s)(g(s) g(t))ds, t [ɛ, a],, t [, ɛ). Moreover, from te Lebesgue dominated convergence teorem, te estimate ( A) 2 β T (t s)(g(s) g(t)) ds (2.9) C 2 β, t > s, (t s) 2 β β and te assumption β + ϑ > 1, follow tat u 1 (t) D (A) for every t [, a] and tat (2.1) t ( A)2 β T (t s)(g(s) g(t))ds, for t >,, for t =,

10 74 Eduardo Hernández since A is a closed operator. Te continuity of Au 1 on [, a] follows from te Lebesgue dominated convergence teorem and inequality (2.9). Te property for u ( ) is proved in usual form. complete. Te proof is Lemma 3. Under te assumptions of Lemma 2, Au 1 C, ν ([, a]; X) for β + ϑ 1 + ν. Proof. At first we observe tat for t > s and ξ (, 1), ( A) 2 ξ T (t) ( A) 2 ξ T (s) t s ( A) 3 ξ T (τ) dτ and ence C 3 ξ t s dτ τ 3 ξ C 3 ξt 1 ξ (t s) t 2 ξ s 2 ξ, (2.11) ( A) 2 ξ T (t) ( A) 2 ξ T (s) C 3 ξ(t s). t 1 ξ s 2 ξ Let δ > and t (δ, a]. Using (2.1), for > we get Au 1 (t + ) Au 1 (t) t ( A)2 β (T (t + s) T (t s))(g(s) g(t)) ds + t ( A) 2 β (2.12) T (t + s)(g(t) g(t + )) ds + t+ t ( A) 2 β T (t + s)(g(s) g(t + )) ds = I 1 (t, ) + I 2 (t, ) + I 3 (t, ). Next we estimate eac I i (t, ) separately. From inequality (2.11)

11 Regularity of Solutions of Partial Neutral Functional 75 we find tat I 1 (t, ) t ( A) 2 β (T (t + s) T (t s))(g(s) g(t)) ds C 3 β ds (t + s) 1 β (t s) 2 β ϑ C 3 β ds (t + s) 1 β (t s) 2 β ϑ t + t t C 3 β β+ϑ 1 t +C 3 β β t t ds (t + s) 1 β ds (t s) 2 β ϑ (2.13) consequently (2.14) c 1 β+ϑ 1 + c 2 2β+ϑ 1, I 1 (t, ) c 3 β+ϑ 1. For te second term we see tat I 1 (t, ) t ( A) 2 β T (t + s)(g(t + ) g(t)) ds c 4 ϑ t ds (t + s) 2 β ϑ c 5, 1 β and ence (2.15) I 2 (t, ) c 5 β+ϑ 1. Similarly, for te tird term we find tat (2.16) I 3 (t, ) c 6 β+ϑ 1. Te assertion is now consequence of (2.12), (2.14), (2.15) and (2.16). Te proof is complete. Proposition 2. Assume tat te assumptions of Lemma 2 old. If u( ) is te mild solution of (2.6), ten te following properties are verified.

12 76 Eduardo Hernández (a) If g C, µ ([, a]; X 1 β ) ten u C, ϱ ([δ, a]; X 1 ) C 1, ϱ ([δ, a]; X) for every δ > and every < ϱ min{µ, β + ϑ 1}. (b) If g C, µ ([, a]; X 1 β ) and g() =, ten u C, ϱ ([, a]; X 1 ) C 1, ϱ ([, a]; X) for every ϱ min{µ, β+ ϑ 1}. (c) If g C([, a]; X 1 β+ν ) ten u C, ϱ ([, a]; X 1 ) C 1 ([, a]; X) for every ϱ < ν. Proof. From Lemma 2, Au C([, a]; X) and t Au(t) = ( A) 2 β T (t s)(g(s) g(t))ds = t t ( A) 2 β T (t s)g(t)ds ( A) 2 β T (t s)(g(s) g(t))ds ( A) 1 β T (t)g(t) + A 1 β g(t) := Au 1 (t) + v(t) + w(t). Next we discuss (a), (b), (c) separately. (a) Let δ >. From te assumptions and Lemma 3, we know tat w C, µ ([, a]; X) and tat Au 1 C, β+ϑ 1 ([, a]; X). On te oter and, since v(t + ) v(t) (T (t + ) T (t))( A) 1 β g(t + ) + ( A) 1 β T (t)(g(t + ) g(t)) te followings inequalities old v (t + ) v (t) c 1 δ c 3 + c 2 ϑ δ 1 β + c δ 4 µ, c 5 v + c 6 ϑ, ν < β δ 1 β+ϑ δ 1 β c 7 ν + c δ 1 β+ϑ 8 µ, ν < β

13 Regularity of Solutions of Partial Neutral Functional 77 and ence v(t + ) v(t) c 3 max{ϑ,µ} Consequently, u C, ϱ ([δ, a]; X) C 1, ϱ ([δ, a]; X) for ϱ min{µ, β + ϑ 1}. (b) As in te previous case, w C, µ ([, a]; X) and Au 1 C β+ϑ 1 ([, a]; X). Moreover, for > we find tat v(t + ) v(t) T (t + )(( A) 1 β g(t + ) ( A) 1 β g(t)) + t+ t AT (s)[( A) 1 β g(t) ( A) 1 β g()] ds T (t + )(( A) 1 β g(t + ) ( A) 1 β g(t)) t+ t c 1 s µ 1 ds c 1 ϑ + c 2 µ, or 1 β c 3 µ, c 4 µ, tus u C, ϱ ([, a]; X 1 ) C 1, ϱ ([, a]; X) for ϱ min{β + ϑ 1, µ}. (c) From Lemma 2, we know tat (2.17) Au(t) = t ( A) 2 β T (t s)g(s)ds, t. Under tis remark, for t [, a], > and ϱ < ν we get Au(t + ) Au(t) t (T () I)( A) 1 ν T (t s)( A) 1 β+ν g(s) ds + t+ t ( A) 1 ν T (t + s)( A) 1 β+ν g(s) ds C ξ ς ( A) 1 β+ν g t ds a (t s) ϱ+1 ν +C ( A) 1 β+ν 1 ν g t+ ds a t ds (t+ s) 1 ν c 1 ϱ + c 2 ν. Tus, u C, ϱ ([, a]; X 1 ) C 1 ([, a]; X) for ϱ < ν. Tis complete te proof. Te following result can be proved using te steps in te proof of Proposition 2. We will omit te proof. δ

14 78 Eduardo Hernández Corollary 1. Let ϑ, β, η (, 1) wit β + ϑ > 1 ; f( ) C, η ([, a]; X) and g( ) C, ϑ ([, a]; X) C([, a]; X 1 β ). If u( ) is te mild solution of (2.18) { x (t) = Ax(t) + A 1 β g(t) + f(t), t [, a], x() =, ten te following properties are verified: (a) u C([, a]; X 1 ) C 1 ([, a], X), (b) If g C, µ ([, a]; X 1 β ) ten u C, ϱ ([δ, a]; X 1 ) C 1, ϱ ([δ, a]; X) for every < ϱ min{µ, β + ϑ 1, η}, (c) If g C, µ ([, a]; X 1 β ) and g() = f() = ten u C,ϱ ([, a]; X 1 ) C 1,ϱ ([, a]; X) for eac < ϱ min{µ, β + ϑ 1, η}, (d) If g C([, a]; X 1 β+ν ) and f C([, a]; X µ ) ten u C, ϱ ([, a]; X 1 ) C 1 ([, a]; X) for every < ϱ < min{µ, ν}. In te rest of tis paper, we always assume tat te functions F, G verifies te ypotesis in Teorem 1.1. Moreover, to simplify our notations, we only consider te case σ =. Now we establis a first result about te existence of regular solutions; specifically we prove existence of N-classical solutions. Teorem 2. Assume tat tere exist constants < α < β < 1; < γ 1, γ 2 1 and an open subset Ω α B α suc tat F : [, a] Ω α X 1 and G : [, a] Ω α X are continuous functions and tat te following conditions old:

15 Regularity of Solutions of Partial Neutral Functional 79 (a) Te function F is X β -valued and tere exist positive constants L i, L i, i = 1, 2, suc tat ( A) β F (t, ψ 1 ) ( A) β F (s, ψ 2 ) L 1 t s γ 1 +L 1 ψ 1 ψ 2 Bα, G(t, ψ 1 ) G(s, ψ 2 ) L 2 t s γ 2 +L 2 ψ 1 ψ 2 Bα, for every s, t a, ψ 1, ψ 2 Ω α. (b) K()L 1 ( A) α β < 1. (c) ϕ Ω α and tere exists < ξ 1 suc tat te function W ( )ϕ is ξ-hölder on [, a]. If β + Min{β α, ξ, γ 1, γ 2 } > 1, ten tere exists a unique N- classical solution x(, ϕ) of te abstract Caucy problem (1.1) defined on (, b), for some < b < a. Proof: From our assumptions on te operator A, see lemma (1), we fix positive constants C α and C α+1 β suc tat for all t (, T ] ( A) α T (t) C α t α and ( A) 1 β+α T (t) C α+1 β t (1 β+α). Let b 1 > and δ > suc tat V = {(s, ψ) : s b 1, ψ ϕ Bα < δ} [, a] Ω α and µ = K b1 ( A) α β L 1 < 1. Now we coose < b < b 1 suc tat (2.19) sup W (θ) ( A) α (ϕ) ( A) α (ϕ) β < [,b] (1 µ) δ, 4 (2.2) K b sup T (θ) ( A) α ϕ () ( A) α ϕ () [,b] < (1 µ) δ, 8

16 8 Eduardo Hernández (2.21) K b sup T (θ) ( A) α f (, ϕ) ( A) α f (, ϕ) [,b] < (1 µ) δ, 4 ( A) α β K b L 1 b γ 1 (1 µ) (2.22) < δ, 8 b β α β α K b C α+1 β {L 1 b γ 1 + L 1 δ+ ( A) β F (, ϕ) < (2.23) b 1 α (2.24) K b 1 α C α{l 2 b γ 2 + L 2 δ+ G(, ϕ) } < (2.25) K b {C α+1 β L 1 (1 µ) δ, 4 b β α β α + C α L b 1 α (1 µ) 2 } < 1 α 2 (1 µ) δ, 4 In te space Y = C([, b] : X) provided wit te topology of uniform convergence, we define; A(ϕ, α, b) = {u Y : u() = ( A) α ϕ(), ( A) α ϕ ũ t B δ, t [, b] }, were ũ is te extension of u to (, b] wit ũ = ( A) α ϕ. From (2.19), it follows tat A(ϕ, α, b) is a nonempty, convex and closed subset of Y. On A(ϕ, α, b) we define te operator Φ by te expression Φ(u)(t) = T (t)(( A) α (ϕ() + F (, ϕ)) ( A) α F (t, ( A) α ũ t ) + t ( A)α+1 β T (t s)( A) β F (s, ( A) α ũ s )ds + t ( A)α T (t s)g(s, ( A) α ũ s )ds In order to use te contraction mapping principle, we now sow tat te range of Φ is included in A(ϕ, α, b). To tis end we introduce te functions y α, z i : (, b] X, i = 1, 2, 3, were y α (t) = T (t)( A) α ϕ for t, (y α ) = ( A) α ϕ and z 1 (t) = T (t)( A) α F (, ϕ) ( A) α F (t, ( A) α ũ t ), z 2 (t) = t ( A)α+1 β T (t s)( A) β F (s, ( A) α ũ s )ds, z 3 (t) = t ( A)α T (t s)g(s, ( A) α ũ s )ds, for t >, z i = for i {1, 2, 3}. Clearly (2.26) Φ(u)(t) = y α (t) + z 1 (t) + z 2 (t) + z 3 (t)

17 Regularity of Solutions of Partial Neutral Functional 81 on [, b] and Φ(u) t = (y α ) t + zt 1 + zt 2 + zt 3. Wit te previous notations, for t [, b] we ave, (2.27) Φ(u) t ( A) α ϕ B (y α ) t ( A) α ϕ B + zt 1 B + zt 2 B + zt 3 B. Using axiom (A) concerning te pase space, we estimate eac term on te rigt and side of (2.27) separately. Directly from te coice of b we get te estimate (2.28) (y α ) t ( A) α ϕ B W (t)( A) α ϕ ( A) α ϕ B On te oter and, for t [, b] (2.29) and for zt 1 (1 µ) δ. 4 K b sup z 1 (s) B s [,t] z 1 (s) T (s)( A) α F (, ϕ) ( A) α F (, ϕ) + ( A) α F (, ϕ) ( A) α F (s, ( A) α ũ s ) (1 µ) δ + L 1 ( A) α β b γ 1 8K b +L 1 ( A) α β ( A) α ϕ ũ s B ence (2.3) z 1 (s) and substituting (2.3) into (2.29) (2.31) 2(1 µ) δ + L 1 ( A) α β δ, 8K b z 1 t B (1 µ) δ + µδ. 4 Now, for te function z 2 ( ) we ave tat (2.32) zt 2 B K b sup z 2 (s) s [,t]

18 82 Eduardo Hernández and for s [, t] z 2 (s) s ( A) α+1 β T (s θ)(( A) β F (θ, ( A) α ũ θ ) ( A) β F (, ϕ)) dθ + s s ( A) α+1 β T (s θ)( A) β F (, ϕ)) dθ C α+1 β (s θ) α+1 β {L 1θ γ1 ũ θ ( A) α ϕ B }}dθ + bβ α β α C α+1 β ( A) β F (, ϕ) (L 1 b γ 1 + L 1 δ) bγ α β α C α+1 β + bβ α β α C α+1 β ( A) β F (, ϕ). Employing te last inequality in (2.32) we obtain tat; (2.33) z 2 t bβ α K { } β α bc α+1 β L1 b γ 1 + L 1δ + ( A) β F (, ϕ) (1 µ) 4 δ. Similarly for z 3, zt 3 b 1 α B K b 1 α C α {L 2 b γ 2 + L (1 µ) 2δ+ G(, ϕ) } δ. 4 (2.34) Combining (2.27), (2.28), (2.31), (2.33) and (2.34), we conclude tat Φ(u) A(ϕ, α, b). Now we prove tat Φ is a contraction. Let u, v A(ϕ, α, b), so tat Φ(u)(t) Φ(v)(t) ( A) α F (t, ( A) α ũ t ) ( A) α F (t, ( A) α ṽ t ) + t ( A) α+1 β T (t s) ( ( A) β F ( s, ( A) α ) ũ s

19 Regularity of Solutions of Partial Neutral Functional 83 ( A) β F ( s, ( A) α ṽ s )) ds + t ( A)α T (t s)(g(s, ( A) α ũ s ) G(s, ( A) α ṽ s )) ds ( A) α β L 1 ũ t ṽ t B + ( t Cα+1 B L 1 (t s) α+1 B + C αl ) 2 (t s) α ũ s ṽ s B ds, tus (2.35) Φ(u) Φ(v) b K b { ( A) α β L 1 +C α+1 β L 1 bβ α + C β α αl 2 b1 α } u v 1 α B. From (2.25), (2.35) and te contraction mapping principle, we can conclude tat Φ as a unique fixed point x( ) in A(ϕ, α, b). From te assumptions on F and G, it follows tat te functions t G(t, ( A) α x t ) and t ( A) β F (t, ( A) α x t ) are continuous and bounded on [, b]. In te following N will be a positive constant suc tat ( A) β F (t, ( A) α x t ) N, G(t, ( A) α x t ) N, for all t [, b]. Next we will prove tat te functions t ( A) β F (t, ( A) α x t ) and t G(t, ( A) α x t ) are Hölder continuous on [, b]. From Lemma 1 and te condition β +Min{β α, ξ, γ 1, γ 2 } > 1, we fix < ϑ < min{β α, ξ, γ 1, γ 2 } wit ϑ + β > 1 and C > suc tat for all < s < t < b 1 and < < 1 (2.36) (2.37) (T () I)( A) α T (t s) C ϑ (t s) (ϑ+α), (T () I)( A) α+1 β T (t s) C ϑ (t s) (α+1 β+ϑ). For t [, b) and < < 1 wit t + < b we get

20 84 Eduardo Hernández x(t + ) x(t) C 1 ξ + C 2 1 α + ( A) α F (t +, ( A) α x t+ ) ( A) α F (t, ( A) α x t ) + t ( A) α+1 β (T () I)T (t s)( A) β F (s, ( A) α x s ) ds + t+ t ( A) α+1 β T (t + s)( A) β F (s, ( A) α x s ) ds + t+ t ( A) α (T () I) T (t s) G (s, ( A) α x s ) ds + t+ t ( A) α T (t + s)g(s, ( A) α x s ) ds. (2.38) We estimate eac term on te rigt and side of te last inequality separately. For te tird term we ave I 3 ( A) α β ( A) β F (t +, ( A) α x t+ ) ( A) β F (t, ( A) α x t ) ( A) α β {L1 γ 1 + L 1 x t+ x t B } ( A) α β L1 γ 1 + ( A) α β L 1M b x ( A) α ϕ B +( A) α β L 1 K b equivalently, sup x(θ + ) x(θ) θ [,t] I 3 C 3 γ 1 + ( A) α β L 1 M b x ( A) α ϕ B (2.39) + ( A) α β L 1 K b sup θ [,t] x(θ + ) x(θ), for some constant C 3, independent of t and. Wit respect to te fourt term, we get I 4 = t (T () I)( A) α+1 β T (t s)( A) β F (s, ( A) α x s ) ds t ϑ N C ds (t s) α+1 β+ϑ tβ α ϑ C N ϑ, β α ϑ

21 Regularity of Solutions of Partial Neutral Functional 85 wic can be abbreviated as (2.4) I 4 C 4 ϑ, were C 4 is a constant independent of t and. For I 5 we find tat I 5 t+ t ten ( A) α+1 β T (t + s)( A) β F (s, ( A) α x s ) ds C α+1 β N β α β α C 5 ϑ (2.41) I 5 C 5 ϑ were C 5 is a constant independent of t [, b) and < < 1. In a similar manner we can prove tat (2.42) I 6 C 6 ϑ and I 7 C 7 ϑ, were C 6 and C 7 are positive constants independents of t [, b) and < < 1. Using te estimates (2.39)-(2.42), tere exists a constant C 1 >, independent of t [, b) suc tat for < < 1 wit < t+ < b, x(t + ) x(t) C 1 ϑ + ( A) α β L 1 M b x ( A) α ϕ B + ( A) α β L 1 K b sup x(θ + ) x (θ) θ [,t] consequently (2.43) x(θ + ) x(θ) [,t] C 1 ϑ 1 µ + M bl 1 1 µ ( A)α β x ( A) α ϕ B since < µ = K b1 ( A) α β L 1 < 1. Moreover, using te definition of y α and te decomposition of x(t) = Φ(x)(t) as

22 86 Eduardo Hernández indicated in (2.26), it is possible to prove tat x ( A) α ϕ B W ()( A) α ϕ ( A) α ϕ B + 3 i=1 z i B C 8 ξ + z 1 B +C 9 ϑ. (2.44) Now from axiom (A) K sup T (s)( A) α F (, ϕ) ( A) α F (s, ( A) α x s ) B z 1 s [,] (2.45) and for s T (s)( A) α F (, ϕ) ( A) α F (s, ( A) α x s ) (2.46) T (s)( A) α F (, ϕ) ( A) α F (, ϕ) +L 1 s γ 1 ( A) α β +L 1 ( A) α β ( A) α ϕ x s B C 1 ( 1 α + γ 1 ) + L 1 ( A) α β ( A) α ϕ x s B. Employing tis last inequality in (2.45), it follows tat: (2.47) z 1 B C 1 K b ( 1 α + γ 1 ) +K b L 1 A α β A α ϕ x τ τ [,]. From (2.47), (2.44), te coice of b and te fact tat ϑ < Min{β α, ξ, γ 1, γ 2 }; for < < 1 we find tat tus (2.48) x τ ( A) α ϕ τ [,] C 11 ϑ +K b L 1 ( A) α β ( A) α ϕ x τ τ [,] x ( A) α ϕ B C 11 1 µ ϑ. Te inequalities (2.48) and (2.43) sow tat tere exists C 12 >, independent of θ [, b) and >, suc tat (2.49) x(θ + ) x(θ) C 12 ϑ

23 Regularity of Solutions of Partial Neutral Functional 87 were ϑ < Min{β α, ξ, γ 1, γ 2 } and ϑ + β > 1. From (2.48), (2.49) and axiom (A) follows tat te functions ( A) β F (t, ( A) α x t ) and G(t, ( A) α x t ) are ϑ-hölder wit ϑ+ β > 1. We know from Corollary (1), tat te abstract Caucy problem (2.5) G(t, ( A) α x t ), w (t) = Aw(t) + ( A) 1 β (( A) β F (t, ( A) α x t )) + x() = ϕ() + F (, ϕ), as a unique classical solution y C((, b]; X 1 ) wic is given by y(t) = T (t)(ϕ() + F (, ϕ)) + t ( A)1 β T (t s)( A) β (2.51) F (s, ( A) α x s )ds + t σ T (t s)g(s, ( A) α x s )ds. Operating on (2.51) wit ( A) α and using te ideas in te proof of Lemma 2, follows tat ( A) α y(t) = x(t)+( A) α F (t, ( A) α x t ), wic in turn implies tat z = ( A) α x C((, b]; X 1 ) since t F (t, x t ) is continuous wit values in X 1. Let z : (, b] X a extension of z suc tat z = ϕ. Clearly, z is a N-classical solution of te neutral problem (1.1). Te proof is complete. Now we turn our attention to te problem of existence of classical solutions. In te rest of tis paper, for a function j : [, a] B X and IR we use te notation j for te function j(t) := j(t +, ψ) j(t, ψ). Moreover, if j is differentiable we will employ te following decomposition (2.52) j(t + s, ψ + ψ 1 ) j(t, ψ) = (D 1 j(t, ψ), D 2 j(t, ψ))(s, ψ 1 ) + (s, ψ 1 ) R(j, t, ψ, s, ψ 1 )

24 88 Eduardo Hernández were (2.53) R(j, t, ψ, s, ψ 1 ) as (s, ψ 1 ). To prove Teorem 3 below, we will employ te following property. Lemma 4. Let X, Y be Banac spaces, Ω X open, K Ω compact and f : Ω X Y be a continuously differentiable function. Ten, for every ɛ > tere exists δ > suc tat f(x) f(y) (D x f)(x y) ɛ x y, for every x, y K suc tat x y < δ. Te next result establises te existence of classical solutions for te neutral system (1.1), making use of usual regularity assumptions for te functions ( A) β F and G. Teorem 3. Let assumptions in Teorem 1 be satisfied. Assume tat ϕ D(A W ), tat ( A) β F and G are continuously differentiable on [, a] Ω, tat F is continuous wit values in X 1 and tat D(( A) β F )(, ϕ). If X G(,ϕ) or X G(,ϕ) B and B satisfies axiom C 3, ten tere exists a unique classical solution of te system (1.1) defined on [, b] for some < b < a. Proof. Let u := u(, ϕ) te mild solution of (1.1). In te following we assume tat u( ) is defined on (, 2b] were < 2b < a and µ = K 2b [ D 2 F (s, u s ) + bβ C 1 β β (2.54) +b M ] D 2 G(s, u s ) 2b < 1. D 2 ( A) β F (s, u s ) Let z( ) be te solution of te integral equation

25 Regularity of Solutions of Partial Neutral Functional 89 (2.55) z(t) = T (t)aϕ() + p(t) D 2 F (t, u t )(z t ) + + t t wit initial condition ( A) 1 β T (t s)[d 2 ( A) β F (s, u s )](z s )ds T (t s)d 2 G(s, u s )(z s )ds, t, (2.56) z = A W (ϕ) + X G(,ϕ), and were p(t) = D 1 F (t, u t ) + + t t ( A) 1 β T (t s)d 1 ( A) β F (s, u s )ds T (t s)d 1 G(s, u s )ds + T (t)g(, ϕ). Te existence and uniqueness of local solution to te integral equation (2.55)-(2.56) is clear and we omit te proof. In wat follows we assume tat z( ) C([, b] : X). We affirm tat u ( ) = z( ) on [, b]. In order to prove te assertion, for t [, b] and < < 1 sufficiently small we ave u (t) z (t) [ T () I T (t) ϕ() Aϕ()] ( ) T () I + T (t) F (, ϕ) + 1 ( A)1 β T (t + s)( A) β F (s, u s ) ds F (t +, u t+ ) + F (t, u t ) + + D 1 F (t, u t ) + D 2 F (t, u t )(z t ) + t C 1 β (t s) 1 β ( A) β F (s, u s ) D 1 ( A) β F (s, u s ) D 2 ( A) β F (s, u s )(z s ds

26 9 Eduardo Hernández 1 + T (t + s)g(s, u s)ds T (t)g(, ϕ) + t M G(s, u s ) D 1 G(s, u s ) D 2 G(s, u s )(z s ) ds Next we use te notations I i (t, ), i = 1,...6, for te terms of te rigt and side of te last inequality. It is clear tat (2.57) I i (t, ), as, i {1, 2, 5} uniformly for t [, b]. On te oter and for te tird term I 3 (t, ) = F (t, u t ) + D 1 F (t, u t ) + D 2 F (t, u t )(z t ) D 2 F (t, u t )( u t+ u t z t ) + (, u t+ u t ) R(F, t, u t,, u t+ u t ). Since te function t x t is Lipscitz continuous on [, b], see Proposition (3.1) in [5], follows from Lemma 4 we get (, u t+ u t )) (2.58) (2.59) R(F, t, u t,, u t+ u t ) as, uniformly for t [, b]. Consequently, we can rewrite te last inequality in te form (2.6) I 3 (t, ) ξ 3 (t, )+ D 2 F (t, u t ) u t+ u t B z t were ξ 3 (t, ) if uniformly for t [, b]. Using similar arguments, we ave for I 4 tat I 4 (t, ) t C 1 β D2 ( A) β F (s, u (t s) 1 β s ) u s+ u s z B s ds + t R(( A) β F, s, u s,, u s+ u s ) ds (,u s+ u s)

27 Regularity of Solutions of Partial Neutral Functional 91 and so, from (2.58) we get I 4 (t, ) ξ 4 (t, ) + t C 1 β D2 ( A) β F (s, u (t s) 1 β s ) (2.61) ( u s+ u s z s ) ds B were ξ 4 (t, ) as uniformly for t [, b]. Analogously, for I 6 we see tat t I 6 (t, ) ξ 6 (t, )+ M D 2 G(s, u s ) (u s+ u s z s ) ds B (2.62) were ξ 6 (t, ) as uniformly for t [, b]. Combining (2.57), (2.6), (2.61), (2.62) and te first inequality we get u(t) z(t) ( ) ut+ u ξ 7 (t, ) + D 2 F (t, u t ) t B z t + t C ( ) 1 β D (t s) 1 β 2 ( A) β us+ u F (s, u s ) s B z s ds + t M ( ) us+ u D 2 G(s, u s ) s B z s ds, were ξ 7 (t, ) as uniformly for t [, b]. Using axiom (A) and (2.54) we infer tat, u( ) z( ) [,t] 1 max 1 µ s [,t] ξ 7 (s, ) + M 2bµ + u ϕ B z. (1 µ)k 2b Clearly u ( ) = z( ) if 1 (u ϕ) z as. Next we will prove tis convergence. For > we consider te decomposition (2.63) ( u ϕ B A W (ϕ) X G(,ϕ) W ()ϕ ϕ z 1 + z 2 A W (ϕ) + B B z 3 + X G(,ϕ) B

28 92 Eduardo Hernández were z i = on (, ] and z 1 (θ) = T (θ)f (, ϕ) F (θ, u θ ) z 2 (θ) = z 3 (θ) = θ θ ( A) 1 β T (θ s)( A) β F (s, u s )ds T (θ s)g(s, u s )ds, for θ [, b]. Let I i (), i = 1, 2, 3, be te terms of te rigt and side of (2.63). Clearly (2.64) I 1 () as, since ϕ D(A W ). On te oter and, in bot X G(,ϕ) = or X G(,ϕ), te ypotesis imply tat (2.65) I 3 () as. For te second term we get (2.66) I 2 () 1 K b (T (θ) I)F (, ϕ) + θ ( A)1 β T (θ s)( A) β F (s, u s )ds 1 +K b F (, ϕ) F (θ, u θ) θ [,]. θ [,] Moreover for θ [, ], 1 (T (θ) I) F (, ϕ) + θ ( A)1 β T (θ s)( A) β F (s, u s )ds 1 θ ( A) 1 β T (θ s){( A) β F (s, u s ) ( A) β F (, ϕ)} ds 1 θ C 1 β L (θ s) (s+ ϕ u 1 β s B )ds 1 C 1 βl( + C) β β

29 Regularity of Solutions of Partial Neutral Functional 93 were we use te Lipscitz continuity of s u s, see Proposition (3.1) in [5]. Consequently 1 (T (θ) I)F (, ϕ) + θ (2.67) Similarly, we can to prove tat (2.68) ( A)1 β T (θ s)( A) β F (s, u s )ds, as. F (, ϕ) F (θ, u θ ) [,] as, since DF (, ϕ). Using (2.67) and (2.68) in (2.66), we conclude tat (2.69) I 2 (). Now, te convergence of 1 (u ϕ) to z follows from (2.64), (2.65), (2.69) and (2.63). We know from Corollary 1, tat te unique mild solution, y( ), of te Caucy problem w (t) = Aw(t) + ( A) 1 β (( A) β F (t, u t )) + G(t, u t ), w () = ϕ() + F (, ϕ), t (, b), is a classical solution. Consequently, y = d dt (u(t) + F (t, u t)) is continuous on [, b] and u(t) D(A) for every t [, b], since ϕ() D(A) and F ([, a] Ω) D(A). Tus u( ) is a classical solution of (1.1). Te proof is complete. Acknowledgement: Te autor wises to tank to te referees for teir comments and suggestions.

30 94 Eduardo Hernández References [1] Goldstein, Jerome A. Semigroups of linear operators and applications. Oxford Matematical Monograps. Te Clarendon Press, Oxford University Press, New York, (1985). [2] Hale, Jack K.; Kato, Junji.(1978) Pase space for retarded equations wit infinite delay. Funkcial. Ekvac. 21, No. 1, pp [3] Hale, Jack K.; Verduyn Lunel, Sjoerd M. Introduction to functional-differential equations. Applied Matematical Sciences, 99. Springer-Verlag, New York, (1993). [4] Hernández, Eduardo; Henríquez, Hernán R. Existence of periodic solutions of partial neutral functional-differential equations wit unbounded delay. J. Mat. Anal. Appl. 221, No. 2, PP , (1998). [5] Hernández, Eduardo; Henríquez, Hernán R. Existence results for partial neutral functional-differential equations wit unbounded delay. J. Mat. Anal. Appl. 221 (1998), no. 2, [6] Henríquez, Hernán R. Regularity of solutions of abstract retarded functional-differential equations wit unbounded delay. Nonlinear Anal. 28, No. 3, pp , (1997). [7] Henríquez, Hernán R. Periodic solutions of quasi-linear partial functional-differential equations wit unbounded delay. Funkcial. Ekvac. 37, No. 2, pp , (1994). [8] Hino, Yosiyuki; Murakami, Satoru; Yosizawa, Taro. Existence of almost periodic solutions of some functionaldifferential equations wit infinite delay in a Banac space. Tôoku Mat. J. (2) 49, No. 1, pp , (1997). [9] Krein, S. G. Linear differential equations in Banac space. Translated from te Russian by J. M. Danskin. Translations of Matematical Monograps, Vol. 29. American Matematical Society, Providence, R. I., (1971).

31 Regularity of Solutions of Partial Neutral Functional 95 [1] Pazy, A. Semigroups of linear operators and applications to partial differential equations. Applied Matematical Sciences, 44. Springer-Verlag, New York-Berlin, (1983). [11] B. N. Sadovskii. On a fixed point principle. Funct. Anal. Appl. 1, pp , (1967). [12] Travis, C. C.; Webb, G. F. Existence and stability for partial functional differential equations. Trans. Amer. Mat. Soc. 2, pp , (1974). Received : December 21.. Eduardo Hernández Instituto de Ciências Matemáticas e de computação Universidade de São Paulo Campus de São Carlos Caixa Postal 668, , São Carlos, SP Brazil lalom@icmc.sc.usp.br.

A SHORT INTRODUCTION TO BANACH LATTICES AND

A SHORT INTRODUCTION TO BANACH LATTICES AND CHAPTER A SHORT INTRODUCTION TO BANACH LATTICES AND POSITIVE OPERATORS In tis capter we give a brief introduction to Banac lattices and positive operators. Most results of tis capter can be found, e.g.,

More information

Impulsive partial neutral differential equations

Impulsive partial neutral differential equations Applied Mathematics Letters 19 (26) 215 222 www.elsevier.com/locate/aml Impulsive partial neutral differential equations Eduardo Hernández M a,, Hernán R. Henríquez b a Departamento de Matemática, ICMC

More information

Influence of the Stepsize on Hyers Ulam Stability of First-Order Homogeneous Linear Difference Equations

Influence of the Stepsize on Hyers Ulam Stability of First-Order Homogeneous Linear Difference Equations International Journal of Difference Equations ISSN 0973-6069, Volume 12, Number 2, pp. 281 302 (2017) ttp://campus.mst.edu/ijde Influence of te Stepsize on Hyers Ulam Stability of First-Order Homogeneous

More information

OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS. Sandra Pinelas and Julio G. Dix

OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS. Sandra Pinelas and Julio G. Dix Opuscula Mat. 37, no. 6 (2017), 887 898 ttp://dx.doi.org/10.7494/opmat.2017.37.6.887 Opuscula Matematica OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS Sandra

More information

Approximate controllability of impulsive neutral functional differential equations with state-dependent delay via fractional operators

Approximate controllability of impulsive neutral functional differential equations with state-dependent delay via fractional operators International Journal of Computer Applications (975 8887) Volume 69 - No. 2, May 23 Approximate controllability of impulsive neutral functional differential equations with state-dependent delay via fractional

More information

Convexity and Smoothness

Convexity and Smoothness Capter 4 Convexity and Smootness 4.1 Strict Convexity, Smootness, and Gateaux Differentiablity Definition 4.1.1. Let X be a Banac space wit a norm denoted by. A map f : X \{0} X \{0}, f f x is called a

More information

Math 161 (33) - Final exam

Math 161 (33) - Final exam Name: Id #: Mat 161 (33) - Final exam Fall Quarter 2015 Wednesday December 9, 2015-10:30am to 12:30am Instructions: Prob. Points Score possible 1 25 2 25 3 25 4 25 TOTAL 75 (BEST 3) Read eac problem carefully.

More information

Subdifferentials of convex functions

Subdifferentials of convex functions Subdifferentials of convex functions Jordan Bell jordan.bell@gmail.com Department of Matematics, University of Toronto April 21, 2014 Wenever we speak about a vector space in tis note we mean a vector

More information

ch (for some fixed positive number c) reaching c

ch (for some fixed positive number c) reaching c GSTF Journal of Matematics Statistics and Operations Researc (JMSOR) Vol. No. September 05 DOI 0.60/s4086-05-000-z Nonlinear Piecewise-defined Difference Equations wit Reciprocal and Cubic Terms Ramadan

More information

Volume 29, Issue 3. Existence of competitive equilibrium in economies with multi-member households

Volume 29, Issue 3. Existence of competitive equilibrium in economies with multi-member households Volume 29, Issue 3 Existence of competitive equilibrium in economies wit multi-member ouseolds Noriisa Sato Graduate Scool of Economics, Waseda University Abstract Tis paper focuses on te existence of

More information

Strongly continuous semigroups

Strongly continuous semigroups Capter 2 Strongly continuous semigroups Te main application of te teory developed in tis capter is related to PDE systems. Tese systems can provide te strong continuity properties only. 2.1 Closed operators

More information

Semigroups of Operators

Semigroups of Operators Lecture 11 Semigroups of Operators In tis Lecture we gater a few notions on one-parameter semigroups of linear operators, confining to te essential tools tat are needed in te sequel. As usual, X is a real

More information

Smooth Superprocess Evolution Equation Solutions

Smooth Superprocess Evolution Equation Solutions International Matematical Forum, 3, 28, no. 14, 645-66 Smoot Superprocess Evolution Equation Solutions Guillaume Leduc American University of Sarja P.O. Box 26666, Sarja, United Arab Emirates gleduc@aus.edu

More information

Differentiation in higher dimensions

Differentiation in higher dimensions Capter 2 Differentiation in iger dimensions 2.1 Te Total Derivative Recall tat if f : R R is a 1-variable function, and a R, we say tat f is differentiable at x = a if and only if te ratio f(a+) f(a) tends

More information

arxiv:math/ v1 [math.ca] 1 Oct 2003

arxiv:math/ v1 [math.ca] 1 Oct 2003 arxiv:mat/0310017v1 [mat.ca] 1 Oct 2003 Cange of Variable for Multi-dimensional Integral 4 Marc 2003 Isidore Fleiscer Abstract Te cange of variable teorem is proved under te sole ypotesis of differentiability

More information

Global Existence of Classical Solutions for a Class Nonlinear Parabolic Equations

Global Existence of Classical Solutions for a Class Nonlinear Parabolic Equations Global Journal of Science Frontier Researc Matematics and Decision Sciences Volume 12 Issue 8 Version 1.0 Type : Double Blind Peer Reviewed International Researc Journal Publiser: Global Journals Inc.

More information

BOUNDARY REGULARITY FOR SOLUTIONS TO THE LINEARIZED MONGE-AMPÈRE EQUATIONS

BOUNDARY REGULARITY FOR SOLUTIONS TO THE LINEARIZED MONGE-AMPÈRE EQUATIONS BOUNDARY REGULARITY FOR SOLUTIONS TO THE LINEARIZED MONGE-AMPÈRE EQUATIONS N. Q. LE AND O. SAVIN Abstract. We obtain boundary Hölder gradient estimates and regularity for solutions to te linearized Monge-Ampère

More information

Existence Results for Multivalued Semilinear Functional Differential Equations

Existence Results for Multivalued Semilinear Functional Differential Equations E extracta mathematicae Vol. 18, Núm. 1, 1 12 (23) Existence Results for Multivalued Semilinear Functional Differential Equations M. Benchohra, S.K. Ntouyas Department of Mathematics, University of Sidi

More information

Convexity and Smoothness

Convexity and Smoothness Capter 4 Convexity and Smootness 4. Strict Convexity, Smootness, and Gateaux Di erentiablity Definition 4... Let X be a Banac space wit a norm denoted by k k. A map f : X \{0}!X \{0}, f 7! f x is called

More information

Massera-type theorem for the existence of C (n) -almost-periodic solutions for partial functional differential equations with infinite delay

Massera-type theorem for the existence of C (n) -almost-periodic solutions for partial functional differential equations with infinite delay Nonlinear Analysis 69 (2008) 1413 1424 www.elsevier.com/locate/na Massera-type theorem for the existence of C (n) -almost-periodic solutions for partial functional differential equations with infinite

More information

FUNDAMENTAL THEOREM OF CALCULUS FOR HENSTOCK -KURZWEIL INTEGRAL

FUNDAMENTAL THEOREM OF CALCULUS FOR HENSTOCK -KURZWEIL INTEGRAL Bulletin of te Maratwada Matematical Society Vol. 14, No. 1, June 2013, Pages 71 80. FUNDAMENTAL THEOREM OF CALCULUS FOR HENSTOCK -KURZWEIL INTEGRAL Anil Pedgaonkar, Institute of Science, Mumbai 400 030,

More information

Poisson Equation in Sobolev Spaces

Poisson Equation in Sobolev Spaces Poisson Equation in Sobolev Spaces OcMountain Dayligt Time. 6, 011 Today we discuss te Poisson equation in Sobolev spaces. It s existence, uniqueness, and regularity. Weak Solution. u = f in, u = g on

More information

Smoothness of solutions with respect to multi-strip integral boundary conditions for nth order ordinary differential equations

Smoothness of solutions with respect to multi-strip integral boundary conditions for nth order ordinary differential equations 396 Nonlinear Analysis: Modelling and Control, 2014, Vol. 19, No. 3, 396 412 ttp://dx.doi.org/10.15388/na.2014.3.6 Smootness of solutions wit respect to multi-strip integral boundary conditions for nt

More information

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015 Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes

More information

ERROR BOUNDS FOR THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BRADLEY J. LUCIER*

ERROR BOUNDS FOR THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BRADLEY J. LUCIER* EO BOUNDS FO THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BADLEY J. LUCIE* Abstract. Te expected error in L ) attimet for Glimm s sceme wen applied to a scalar conservation law is bounded by + 2 ) ) /2 T

More information

arxiv: v1 [math.dg] 4 Feb 2015

arxiv: v1 [math.dg] 4 Feb 2015 CENTROID OF TRIANGLES ASSOCIATED WITH A CURVE arxiv:1502.01205v1 [mat.dg] 4 Feb 2015 Dong-Soo Kim and Dong Seo Kim Abstract. Arcimedes sowed tat te area between a parabola and any cord AB on te parabola

More information

THE DISCRETE PLATEAU PROBLEM: CONVERGENCE RESULTS

THE DISCRETE PLATEAU PROBLEM: CONVERGENCE RESULTS MATHEMATICS OF COMPUTATION Volume 00, Number 0, Pages 000 000 S 0025-5718XX0000-0 THE DISCRETE PLATEAU PROBLEM: CONVERGENCE RESULTS GERHARD DZIUK AND JOHN E. HUTCHINSON Abstract. We solve te problem of

More information

Lyapunov characterization of input-to-state stability for semilinear control systems over Banach spaces

Lyapunov characterization of input-to-state stability for semilinear control systems over Banach spaces Lyapunov caracterization of input-to-state stability for semilinear control systems over Banac spaces Andrii Mironcenko a, Fabian Wirt a a Faculty of Computer Science and Matematics, University of Passau,

More information

Quasiperiodic phenomena in the Van der Pol - Mathieu equation

Quasiperiodic phenomena in the Van der Pol - Mathieu equation Quasiperiodic penomena in te Van der Pol - Matieu equation F. Veerman and F. Verulst Department of Matematics, Utrect University P.O. Box 80.010, 3508 TA Utrect Te Neterlands April 8, 009 Abstract Te Van

More information

More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms

More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms More on generalized inverses of partitioned matrices wit anaciewicz-scur forms Yongge Tian a,, Yosio Takane b a Cina Economics and Management cademy, Central University of Finance and Economics, eijing,

More information

ANALYTIC SMOOTHING EFFECT FOR THE CUBIC HYPERBOLIC SCHRÖDINGER EQUATION IN TWO SPACE DIMENSIONS

ANALYTIC SMOOTHING EFFECT FOR THE CUBIC HYPERBOLIC SCHRÖDINGER EQUATION IN TWO SPACE DIMENSIONS Electronic Journal of Differential Equations, Vol. 2016 2016), No. 34, pp. 1 8. ISSN: 1072-6691. URL: ttp://ejde.mat.txstate.edu or ttp://ejde.mat.unt.edu ftp ejde.mat.txstate.edu ANALYTIC SMOOTHING EFFECT

More information

Gradient Descent etc.

Gradient Descent etc. 1 Gradient Descent etc EE 13: Networked estimation and control Prof Kan) I DERIVATIVE Consider f : R R x fx) Te derivative is defined as d fx) = lim dx fx + ) fx) Te cain rule states tat if d d f gx) )

More information

Function Composition and Chain Rules

Function Composition and Chain Rules Function Composition and s James K. Peterson Department of Biological Sciences and Department of Matematical Sciences Clemson University Marc 8, 2017 Outline 1 Function Composition and Continuity 2 Function

More information

Packing polynomials on multidimensional integer sectors

Packing polynomials on multidimensional integer sectors Pacing polynomials on multidimensional integer sectors Luis B Morales IIMAS, Universidad Nacional Autónoma de México, Ciudad de México, 04510, México lbm@unammx Submitted: Jun 3, 015; Accepted: Sep 8,

More information

A Hybrid Mixed Discontinuous Galerkin Finite Element Method for Convection-Diffusion Problems

A Hybrid Mixed Discontinuous Galerkin Finite Element Method for Convection-Diffusion Problems A Hybrid Mixed Discontinuous Galerkin Finite Element Metod for Convection-Diffusion Problems Herbert Egger Joacim Scöberl We propose and analyse a new finite element metod for convection diffusion problems

More information

EXISTENCE OF SOLUTIONS FOR A SECOND ORDER ABSTRACT FUNCTIONAL DIFFERENTIAL EQUATION WITH STATE-DEPENDENT DELAY

EXISTENCE OF SOLUTIONS FOR A SECOND ORDER ABSTRACT FUNCTIONAL DIFFERENTIAL EQUATION WITH STATE-DEPENDENT DELAY Electronic Journal of Differential Equations, Vol. 27(27), No. 21, pp. 1 1. ISSN: 172-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) EXISTENCE

More information

called the homomorphism induced by the inductive limit. One verifies that the diagram

called the homomorphism induced by the inductive limit. One verifies that the diagram Inductive limits of C -algebras 51 sequences {a n } suc tat a n, and a n 0. If A = A i for all i I, ten A i = C b (I,A) and i I A i = C 0 (I,A). i I 1.10 Inductive limits of C -algebras Definition 1.10.1

More information

CELL CENTERED FINITE VOLUME METHODS USING TAYLOR SERIES EXPANSION SCHEME WITHOUT FICTITIOUS DOMAINS

CELL CENTERED FINITE VOLUME METHODS USING TAYLOR SERIES EXPANSION SCHEME WITHOUT FICTITIOUS DOMAINS INTERNATIONAL JOURNAL OF NUMERICAL ANALYSIS AND MODELING Volume 7, Number 1, Pages 1 9 c 010 Institute for Scientific Computing and Information CELL CENTERED FINITE VOLUME METHODS USING TAYLOR SERIES EXPANSION

More information

LEAST-SQUARES FINITE ELEMENT APPROXIMATIONS TO SOLUTIONS OF INTERFACE PROBLEMS

LEAST-SQUARES FINITE ELEMENT APPROXIMATIONS TO SOLUTIONS OF INTERFACE PROBLEMS SIAM J. NUMER. ANAL. c 998 Society for Industrial Applied Matematics Vol. 35, No., pp. 393 405, February 998 00 LEAST-SQUARES FINITE ELEMENT APPROXIMATIONS TO SOLUTIONS OF INTERFACE PROBLEMS YANZHAO CAO

More information

EXISTENCE THEOREMS FOR FUNCTIONAL DIFFERENTIAL EQUATIONS IN BANACH SPACES. 1. Introduction

EXISTENCE THEOREMS FOR FUNCTIONAL DIFFERENTIAL EQUATIONS IN BANACH SPACES. 1. Introduction Acta Math. Univ. Comenianae Vol. LXXVIII, 2(29), pp. 287 32 287 EXISTENCE THEOREMS FOR FUNCTIONAL DIFFERENTIAL EQUATIONS IN BANACH SPACES A. SGHIR Abstract. This paper concernes with the study of existence

More information

Math Spring 2013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, (1/z) 2 (1/z 1) 2 = lim

Math Spring 2013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, (1/z) 2 (1/z 1) 2 = lim Mat 311 - Spring 013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, 013 Question 1. [p 56, #10 (a)] 4z Use te teorem of Sec. 17 to sow tat z (z 1) = 4. We ave z 4z (z 1) = z 0 4 (1/z) (1/z

More information

University Mathematics 2

University Mathematics 2 University Matematics 2 1 Differentiability In tis section, we discuss te differentiability of functions. Definition 1.1 Differentiable function). Let f) be a function. We say tat f is differentiable at

More information

Research Article Existence of the Mild Solutions for Impulsive Fractional Equations with Infinite Delay

Research Article Existence of the Mild Solutions for Impulsive Fractional Equations with Infinite Delay International Journal of Differential Equations Volume 211, Article ID 79323, 2 pages doi:1.1155/211/79323 Researc Article Existence of te Mild Solutions for Impulsive Fractional Equations wit Infinite

More information

On convexity of polynomial paths and generalized majorizations

On convexity of polynomial paths and generalized majorizations On convexity of polynomial pats and generalized majorizations Marija Dodig Centro de Estruturas Lineares e Combinatórias, CELC, Universidade de Lisboa, Av. Prof. Gama Pinto 2, 1649-003 Lisboa, Portugal

More information

Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series

Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series Lawrence D. Brown, Pilip A. Ernst, Larry Sepp, and Robert Wolpert August 27, 2015 Abstract We consider te class,

More information

Copyright 2012 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future

Copyright 2012 IEEE. Personal use of this material is permitted. Permission from IEEE must be obtained for all other uses, in any current or future Copyrigt 212 IEEE. Personal use of tis material is permitted. Permission from IEEE must be obtained for all oter uses, in any current or future media, including reprinting/republising tis material for

More information

FINITE ELEMENT APPROXIMATIONS AND THE DIRICHLET PROBLEM FOR SURFACES OF PRESCRIBED MEAN CURVATURE

FINITE ELEMENT APPROXIMATIONS AND THE DIRICHLET PROBLEM FOR SURFACES OF PRESCRIBED MEAN CURVATURE FINITE ELEMENT APPROXIMATIONS AND THE DIRICHLET PROBLEM FOR SURFACES OF PRESCRIBED MEAN CURVATURE GERHARD DZIUK AND JOHN E. HUTCHINSON Abstract. We give a finite element procedure for te Diriclet Problem

More information

GELFAND S PROOF OF WIENER S THEOREM

GELFAND S PROOF OF WIENER S THEOREM GELFAND S PROOF OF WIENER S THEOREM S. H. KULKARNI 1. Introduction Te following teorem was proved by te famous matematician Norbert Wiener. Wiener s proof can be found in is book [5]. Teorem 1.1. (Wiener

More information

NOTES ON LINEAR SEMIGROUPS AND GRADIENT FLOWS

NOTES ON LINEAR SEMIGROUPS AND GRADIENT FLOWS NOTES ON LINEAR SEMIGROUPS AND GRADIENT FLOWS F. MAGGI Tese notes ave been written in occasion of te course Partial Differential Equations II eld by te autor at te University of Texas at Austin. Tey are

More information

Derivatives of Exponentials

Derivatives of Exponentials mat 0 more on derivatives: day 0 Derivatives of Eponentials Recall tat DEFINITION... An eponential function as te form f () =a, were te base is a real number a > 0. Te domain of an eponential function

More information

ERROR ESTIMATES FOR A FULLY DISCRETIZED SCHEME TO A CAHN-HILLIARD PHASE-FIELD MODEL FOR TWO-PHASE INCOMPRESSIBLE FLOWS

ERROR ESTIMATES FOR A FULLY DISCRETIZED SCHEME TO A CAHN-HILLIARD PHASE-FIELD MODEL FOR TWO-PHASE INCOMPRESSIBLE FLOWS ERROR ESTIMATES FOR A FULLY DISCRETIZED SCHEME TO A CAHN-HILLIARD PHASE-FIELD MODEL FOR TWO-PHASE INCOMPRESSIBLE FLOWS YONGYONG CAI, AND JIE SHEN Abstract. We carry out in tis paper a rigorous error analysis

More information

Approximation of the Viability Kernel

Approximation of the Viability Kernel Approximation of te Viability Kernel Patrick Saint-Pierre CEREMADE, Université Paris-Daupine Place du Marécal de Lattre de Tassigny 75775 Paris cedex 16 26 october 1990 Abstract We study recursive inclusions

More information

An approximation method using approximate approximations

An approximation method using approximate approximations Applicable Analysis: An International Journal Vol. 00, No. 00, September 2005, 1 13 An approximation metod using approximate approximations FRANK MÜLLER and WERNER VARNHORN, University of Kassel, Germany,

More information

HOMEWORK HELP 2 FOR MATH 151

HOMEWORK HELP 2 FOR MATH 151 HOMEWORK HELP 2 FOR MATH 151 Here we go; te second round of omework elp. If tere are oters you would like to see, let me know! 2.4, 43 and 44 At wat points are te functions f(x) and g(x) = xf(x)continuous,

More information

1. Introduction. Consider a semilinear parabolic equation in the form

1. Introduction. Consider a semilinear parabolic equation in the form A POSTERIORI ERROR ESTIMATION FOR PARABOLIC PROBLEMS USING ELLIPTIC RECONSTRUCTIONS. I: BACKWARD-EULER AND CRANK-NICOLSON METHODS NATALIA KOPTEVA AND TORSTEN LINSS Abstract. A semilinear second-order parabolic

More information

On the fixed point theorem of Krasnoselskii and Sobolev

On the fixed point theorem of Krasnoselskii and Sobolev Electronic Journal of Qualitative Theory of Differential Equations 2011, No. 5, 1-6; http://www.math.u-szeged.hu/ejqtde/ On the fixed point theorem of Krasnoselskii and Sobolev Cristina G. Fuentes and

More information

Parameter Dependent Quasi-Linear Parabolic Equations

Parameter Dependent Quasi-Linear Parabolic Equations CADERNOS DE MATEMÁTICA 4, 39 33 October (23) ARTIGO NÚMERO SMA#79 Parameter Dependent Quasi-Linear Parabolic Equations Cláudia Buttarello Gentile Departamento de Matemática, Universidade Federal de São

More information

DIFFERENTIAL POLYNOMIALS GENERATED BY SECOND ORDER LINEAR DIFFERENTIAL EQUATIONS

DIFFERENTIAL POLYNOMIALS GENERATED BY SECOND ORDER LINEAR DIFFERENTIAL EQUATIONS Journal o Applied Analysis Vol. 14, No. 2 2008, pp. 259 271 DIFFERENTIAL POLYNOMIALS GENERATED BY SECOND ORDER LINEAR DIFFERENTIAL EQUATIONS B. BELAÏDI and A. EL FARISSI Received December 5, 2007 and,

More information

A CLASS OF EVEN DEGREE SPLINES OBTAINED THROUGH A MINIMUM CONDITION

A CLASS OF EVEN DEGREE SPLINES OBTAINED THROUGH A MINIMUM CONDITION STUDIA UNIV. BABEŞ BOLYAI, MATHEMATICA, Volume XLVIII, Number 3, September 2003 A CLASS OF EVEN DEGREE SPLINES OBTAINED THROUGH A MINIMUM CONDITION GH. MICULA, E. SANTI, AND M. G. CIMORONI Dedicated to

More information

Decay of solutions of wave equations with memory

Decay of solutions of wave equations with memory Proceedings of te 14t International Conference on Computational and Matematical Metods in Science and Engineering, CMMSE 14 3 7July, 14. Decay of solutions of wave equations wit memory J. A. Ferreira 1,

More information

Weierstraß-Institut. im Forschungsverbund Berlin e.v. Preprint ISSN

Weierstraß-Institut. im Forschungsverbund Berlin e.v. Preprint ISSN Weierstraß-Institut für Angewandte Analysis und Stocastik im Forscungsverbund Berlin e.v. Preprint ISSN 0946 8633 Stability of infinite dimensional control problems wit pointwise state constraints Micael

More information

Error estimates for a semi-implicit fully discrete finite element scheme for the mean curvature flow of graphs

Error estimates for a semi-implicit fully discrete finite element scheme for the mean curvature flow of graphs Interfaces and Free Boundaries 2, 2000 34 359 Error estimates for a semi-implicit fully discrete finite element sceme for te mean curvature flow of graps KLAUS DECKELNICK Scool of Matematical Sciences,

More information

Superconvergence of energy-conserving discontinuous Galerkin methods for. linear hyperbolic equations. Abstract

Superconvergence of energy-conserving discontinuous Galerkin methods for. linear hyperbolic equations. Abstract Superconvergence of energy-conserving discontinuous Galerkin metods for linear yperbolic equations Yong Liu, Ci-Wang Su and Mengping Zang 3 Abstract In tis paper, we study superconvergence properties of

More information

COMPACTNESS PROPERTIES OF THE DG AND CG TIME STEPPING SCHEMES FOR PARABOLIC EQUATIONS. u t + A(u) = f(u).

COMPACTNESS PROPERTIES OF THE DG AND CG TIME STEPPING SCHEMES FOR PARABOLIC EQUATIONS. u t + A(u) = f(u). COMPACTNESS PROPERTIES OF THE DG AND CG TIME STEPPING SCHEMES FOR PARABOLIC EQUATIONS NOEL J. WALKINGTON Abstract. It is sown tat for a broad class of equations tat numerical solutions computed using te

More information

Finite Difference Method

Finite Difference Method Capter 8 Finite Difference Metod 81 2nd order linear pde in two variables General 2nd order linear pde in two variables is given in te following form: L[u] = Au xx +2Bu xy +Cu yy +Du x +Eu y +Fu = G According

More information

On the best approximation of function classes from values on a uniform grid in the real line

On the best approximation of function classes from values on a uniform grid in the real line Proceedings of te 5t WSEAS Int Conf on System Science and Simulation in Engineering, Tenerife, Canary Islands, Spain, December 16-18, 006 459 On te best approximation of function classes from values on

More information

Numerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for Second-Order Elliptic Problems

Numerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for Second-Order Elliptic Problems Applied Matematics, 06, 7, 74-8 ttp://wwwscirporg/journal/am ISSN Online: 5-7393 ISSN Print: 5-7385 Numerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for

More information

arxiv: v1 [math.na] 17 Jul 2014

arxiv: v1 [math.na] 17 Jul 2014 Div First-Order System LL* FOSLL* for Second-Order Elliptic Partial Differential Equations Ziqiang Cai Rob Falgout Sun Zang arxiv:1407.4558v1 [mat.na] 17 Jul 2014 February 13, 2018 Abstract. Te first-order

More information

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator. Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative

More information

The Derivative as a Function

The Derivative as a Function Section 2.2 Te Derivative as a Function 200 Kiryl Tsiscanka Te Derivative as a Function DEFINITION: Te derivative of a function f at a number a, denoted by f (a), is if tis limit exists. f (a) f(a + )

More information

Solutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014

Solutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014 Solutions to te Multivariable Calculus and Linear Algebra problems on te Compreensive Examination of January 3, 24 Tere are 9 problems ( points eac, totaling 9 points) on tis portion of te examination.

More information

Numerical analysis of a free piston problem

Numerical analysis of a free piston problem MATHEMATICAL COMMUNICATIONS 573 Mat. Commun., Vol. 15, No. 2, pp. 573-585 (2010) Numerical analysis of a free piston problem Boris Mua 1 and Zvonimir Tutek 1, 1 Department of Matematics, University of

More information

AN ANALYSIS OF THE EMBEDDED DISCONTINUOUS GALERKIN METHOD FOR SECOND ORDER ELLIPTIC PROBLEMS

AN ANALYSIS OF THE EMBEDDED DISCONTINUOUS GALERKIN METHOD FOR SECOND ORDER ELLIPTIC PROBLEMS AN ANALYSIS OF THE EMBEDDED DISCONTINUOUS GALERKIN METHOD FOR SECOND ORDER ELLIPTIC PROBLEMS BERNARDO COCKBURN, JOHNNY GUZMÁN, SEE-CHEW SOON, AND HENRYK K. STOLARSKI Abstract. Te embedded discontinuous

More information

FINITE DIFFERENCE APPROXIMATIONS FOR NONLINEAR FIRST ORDER PARTIAL DIFFERENTIAL EQUATIONS

FINITE DIFFERENCE APPROXIMATIONS FOR NONLINEAR FIRST ORDER PARTIAL DIFFERENTIAL EQUATIONS UNIVERSITATIS IAGELLONICAE ACTA MATHEMATICA, FASCICULUS XL 2002 FINITE DIFFERENCE APPROXIMATIONS FOR NONLINEAR FIRST ORDER PARTIAL DIFFERENTIAL EQUATIONS by Anna Baranowska Zdzis law Kamont Abstract. Classical

More information

Weak Solutions for Nonlinear Parabolic Equations with Variable Exponents

Weak Solutions for Nonlinear Parabolic Equations with Variable Exponents Communications in Matematics 25 217) 55 7 Copyrigt c 217 Te University of Ostrava 55 Weak Solutions for Nonlinear Parabolic Equations wit Variable Exponents Lingeswaran Sangerganes, Arumugam Gurusamy,

More information

Recent Advances in Time-Domain Maxwell s Equations in Metamaterials

Recent Advances in Time-Domain Maxwell s Equations in Metamaterials Recent Advances in Time-Domain Maxwell s Equations in Metamaterials Yunqing Huang 1, and Jicun Li, 1 Hunan Key Laboratory for Computation and Simulation in Science and Engineering, Xiangtan University,

More information

INNER FUNCTIONS IN THE HYPERBOLIC LITTLE BLOCH CLASS. Wayne Smith

INNER FUNCTIONS IN THE HYPERBOLIC LITTLE BLOCH CLASS. Wayne Smith INNER FUNCTIONS IN THE HYPERBOLIC LITTLE BLOCH CLASS Wayne Smit Abstract. An analytic function ϕ mapping te unit disk into itself is said to belong to te yperbolic little Bloc class if te ratio (1 z 2

More information

1. Questions (a) through (e) refer to the graph of the function f given below. (A) 0 (B) 1 (C) 2 (D) 4 (E) does not exist

1. Questions (a) through (e) refer to the graph of the function f given below. (A) 0 (B) 1 (C) 2 (D) 4 (E) does not exist Mat 1120 Calculus Test 2. October 18, 2001 Your name Te multiple coice problems count 4 points eac. In te multiple coice section, circle te correct coice (or coices). You must sow your work on te oter

More information

Continuity and Differentiability of the Trigonometric Functions

Continuity and Differentiability of the Trigonometric Functions [Te basis for te following work will be te definition of te trigonometric functions as ratios of te sides of a triangle inscribed in a circle; in particular, te sine of an angle will be defined to be te

More information

Numerical Differentiation

Numerical Differentiation Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function

More information

Math 1241 Calculus Test 1

Math 1241 Calculus Test 1 February 4, 2004 Name Te first nine problems count 6 points eac and te final seven count as marked. Tere are 120 points available on tis test. Multiple coice section. Circle te correct coice(s). You do

More information

CONVERGENCE ANALYSIS OF YEE SCHEMES FOR MAXWELL S EQUATIONS IN DEBYE AND LORENTZ DISPERSIVE MEDIA

CONVERGENCE ANALYSIS OF YEE SCHEMES FOR MAXWELL S EQUATIONS IN DEBYE AND LORENTZ DISPERSIVE MEDIA INTRNATIONAL JOURNAL OF NUMRICAL ANALYSIS AND MODLING Volume XX Number 0 ages 45 c 03 Institute for Scientific Computing and Information CONVRGNC ANALYSIS OF Y SCHMS FOR MAXWLL S QUATIONS IN DBY AND LORNTZ

More information

Topics in Generalized Differentiation

Topics in Generalized Differentiation Topics in Generalized Differentiation J. Marsall As Abstract Te course will be built around tree topics: ) Prove te almost everywere equivalence of te L p n-t symmetric quantum derivative and te L p Peano

More information

MIXED DISCONTINUOUS GALERKIN APPROXIMATION OF THE MAXWELL OPERATOR. SIAM J. Numer. Anal., Vol. 42 (2004), pp

MIXED DISCONTINUOUS GALERKIN APPROXIMATION OF THE MAXWELL OPERATOR. SIAM J. Numer. Anal., Vol. 42 (2004), pp MIXED DISCONTINUOUS GALERIN APPROXIMATION OF THE MAXWELL OPERATOR PAUL HOUSTON, ILARIA PERUGIA, AND DOMINI SCHÖTZAU SIAM J. Numer. Anal., Vol. 4 (004), pp. 434 459 Abstract. We introduce and analyze a

More information

A Mixed-Hybrid-Discontinuous Galerkin Finite Element Method for Convection-Diffusion Problems

A Mixed-Hybrid-Discontinuous Galerkin Finite Element Method for Convection-Diffusion Problems A Mixed-Hybrid-Discontinuous Galerkin Finite Element Metod for Convection-Diffusion Problems Herbert Egger Joacim Scöberl We propose and analyse a new finite element metod for convection diffusion problems

More information

A method for solving first order fuzzy differential equation

A method for solving first order fuzzy differential equation Available online at ttp://ijim.srbiau.ac.ir/ Int. J. Industrial Matematics (ISSN 2008-5621) Vol. 5, No. 3, 2013 Article ID IJIM-00250, 7 pages Researc Article A metod for solving first order fuzzy differential

More information

Part VIII, Chapter 39. Fluctuation-based stabilization Model problem

Part VIII, Chapter 39. Fluctuation-based stabilization Model problem Part VIII, Capter 39 Fluctuation-based stabilization Tis capter presents a unified analysis of recent stabilization tecniques for te standard Galerkin approximation of first-order PDEs using H 1 - conforming

More information

Convergence of Rothe s Method for Fully Nonlinear Parabolic Equations

Convergence of Rothe s Method for Fully Nonlinear Parabolic Equations Te Journal of Geometric Analysis Volume 15, Number 3, 2005 Convergence of Rote s Metod for Fully Nonlinear Parabolic Equations By Ivan Blank and Penelope Smit ABSTRACT. Convergence of Rote s metod for

More information

Dedicated to the 70th birthday of Professor Lin Qun

Dedicated to the 70th birthday of Professor Lin Qun Journal of Computational Matematics, Vol.4, No.3, 6, 4 44. ACCELERATION METHODS OF NONLINEAR ITERATION FOR NONLINEAR PARABOLIC EQUATIONS Guang-wei Yuan Xu-deng Hang Laboratory of Computational Pysics,

More information

Overlapping domain decomposition methods for elliptic quasi-variational inequalities related to impulse control problem with mixed boundary conditions

Overlapping domain decomposition methods for elliptic quasi-variational inequalities related to impulse control problem with mixed boundary conditions Proc. Indian Acad. Sci. (Mat. Sci.) Vol. 121, No. 4, November 2011, pp. 481 493. c Indian Academy of Sciences Overlapping domain decomposition metods for elliptic quasi-variational inequalities related

More information

Nonlinear elliptic-parabolic problems

Nonlinear elliptic-parabolic problems Nonlinear elliptic-parabolic problems Inwon C. Kim and Norbert Požár Abstract We introduce a notion of viscosity solutions for a general class of elliptic-parabolic pase transition problems. Tese include

More information

POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY

POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY APPLICATIONES MATHEMATICAE 36, (29), pp. 2 Zbigniew Ciesielski (Sopot) Ryszard Zieliński (Warszawa) POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY Abstract. Dvoretzky

More information

EFFICIENCY OF MODEL-ASSISTED REGRESSION ESTIMATORS IN SAMPLE SURVEYS

EFFICIENCY OF MODEL-ASSISTED REGRESSION ESTIMATORS IN SAMPLE SURVEYS Statistica Sinica 24 2014, 395-414 doi:ttp://dx.doi.org/10.5705/ss.2012.064 EFFICIENCY OF MODEL-ASSISTED REGRESSION ESTIMATORS IN SAMPLE SURVEYS Jun Sao 1,2 and Seng Wang 3 1 East Cina Normal University,

More information

ATTRACTORS FOR SEMILINEAR PARABOLIC PROBLEMS WITH DIRICHLET BOUNDARY CONDITIONS IN VARYING DOMAINS. Emerson A. M. de Abreu Alexandre N.

ATTRACTORS FOR SEMILINEAR PARABOLIC PROBLEMS WITH DIRICHLET BOUNDARY CONDITIONS IN VARYING DOMAINS. Emerson A. M. de Abreu Alexandre N. ATTRACTORS FOR SEMILINEAR PARABOLIC PROBLEMS WITH DIRICHLET BOUNDARY CONDITIONS IN VARYING DOMAINS Emerson A. M. de Abreu Alexandre N. Carvalho Abstract Under fairly general conditions one can prove that

More information

Symmetry Labeling of Molecular Energies

Symmetry Labeling of Molecular Energies Capter 7. Symmetry Labeling of Molecular Energies Notes: Most of te material presented in tis capter is taken from Bunker and Jensen 1998, Cap. 6, and Bunker and Jensen 2005, Cap. 7. 7.1 Hamiltonian Symmetry

More information

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note

More information

arxiv: v1 [math.na] 28 Apr 2017

arxiv: v1 [math.na] 28 Apr 2017 THE SCOTT-VOGELIUS FINITE ELEMENTS REVISITED JOHNNY GUZMÁN AND L RIDGWAY SCOTT arxiv:170500020v1 [matna] 28 Apr 2017 Abstract We prove tat te Scott-Vogelius finite elements are inf-sup stable on sape-regular

More information

CONVERGENCE ANALYSIS OF YEE SCHEMES FOR MAXWELL S EQUATIONS IN DEBYE AND LORENTZ DISPERSIVE MEDIA

CONVERGENCE ANALYSIS OF YEE SCHEMES FOR MAXWELL S EQUATIONS IN DEBYE AND LORENTZ DISPERSIVE MEDIA INTRNATIONAL JOURNAL OF NUMRICAL ANALYSIS AND MODLING Volume Number 4 ages 657 687 c 04 Institute for Scientific Computing and Information CONVRGNC ANALYSIS OF Y SCHMS FOR MAXWLL S QUATIONS IN DBY AND

More information

Blanca Bujanda, Juan Carlos Jorge NEW EFFICIENT TIME INTEGRATORS FOR NON-LINEAR PARABOLIC PROBLEMS

Blanca Bujanda, Juan Carlos Jorge NEW EFFICIENT TIME INTEGRATORS FOR NON-LINEAR PARABOLIC PROBLEMS Opuscula Matematica Vol. 26 No. 3 26 Blanca Bujanda, Juan Carlos Jorge NEW EFFICIENT TIME INTEGRATORS FOR NON-LINEAR PARABOLIC PROBLEMS Abstract. In tis work a new numerical metod is constructed for time-integrating

More information

Andrea Braides, Anneliese Defranceschi and Enrico Vitali. Introduction

Andrea Braides, Anneliese Defranceschi and Enrico Vitali. Introduction HOMOGENIZATION OF FREE DISCONTINUITY PROBLEMS Andrea Braides, Anneliese Defrancesci and Enrico Vitali Introduction Following Griffit s teory, yperelastic brittle media subject to fracture can be modeled

More information