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AIMS’ Journals

Volume X, Number 0X, XX 200X pp. X–XX

HIGH ORDER PERIODIC IMPULSIVE PROBLEMS

Jo˜ao Fialho

School of Mathematics, Physics and Technology College of the Bahamas

Nassau, BAHAMAS

Research Centre on Mathematics and Applications of the University of ´Evora - (CIMA)-UE University of ´Evora, PORTUGAL

Feliz Minh´os Departamento de Matem´atica

Centro de Investiga¸c˜ao em Matem´atica e Aplica¸c˜oes - (CIMA)-UE Escola de Ciˆencias e Tecnologia

Universidade de ´Evora.

Rua Rom˜ao Ramalho, 59, 7000-671 ´Evora, PORTUGAL (Communicated by the associate editor name)

Abstract. The theory of impulsive problem is experiencing a rapid develop-ment in the last few years. Mainly because they have been used to describe some phenomena, arising from different disciplines like physics or biology, sub-ject to instantaneous change at some time instants called moments. Second order periodic impulsive problems were studied to some extent, however very few papers were dedicated to the study of third and higher order impulsive problems.

The high order impulsive problem considered is composed by the fully non-linear equation

u(n)(x) = f x, u (x) , u0(x) , ..., u(n−1)(x)

for a. e. x ∈ I := [0, 1] \ {x1, ..., xm} where f : [0, 1] × Rn → R is L1

-Carath´eodory function, along with the periodic boundary conditions u(i)(0) = u(i)(1) , i = 0, ..., n − 1,

and the impulsive conditions u(i) x+

j = gij(u (xj)) , i = 0, ..., n − 1,

where gi

j, for j = 1, ..., m, are given real valued functions satisfying some

ade-quate conditions, and xj∈ (0, 1) , such that 0 = x0< x1< ... < xm< xm+1=

1.

The arguments applied make use of the lower and upper solution method combined with an iterative technique, which is not necessarily monotone, to-gether with classical results such as Lebesgue Dominated Convergence Theo-rem, Ascoli-Arz`ela Theorem and fixed point theory.

2010 Mathematics Subject Classification. Primary: 34A37; Secondary: 34B15.

Key words and phrases. Higher order problems, Differential equations with impulses, periodic boundary value problems, Nagumo condition, lower and upper solutions.

The authors are partially supported by Funda¸c˜ao para a Ciˆencia e Tecnologia, PEst-OE/MAT/UI0117/2014.

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1. Introduction. Problems with impulses have been experiencing a rapid deve-olpement in the last few years. Their high aplicability in such different disciplines like physics, biology or finance is, most likely, one of the main reasons for that. The problem covered in this paper is a generalization to n − th order of a periodic problem, with some impulses. First and second order periodic impulsive problems were studied to some extent, ([2,3,5,6, 7, 8]), however very few papers were de-dicated to the study of third and higher order impulsive problems. One can refer for instance ([1,4,9]) and the references therein. To the best of our knowledge, no paper generalizes and extends the results to higher order.

We consider the high order impulsive problem composed by the fully nonlinear equation

u(n)(x) = f³x, u (x) , u0(x) , ..., u(n−1)(x)´ (1) for a. e. x ∈ [0, 1] \ {x1, ..., xm} where f : [0, 1] × Rn → R is L1-Carath´eodory function, along with the periodic boundary conditions

u(i)(0) = u(i)(1) , i = 0, ..., n − 1, (2) and the impulsive conditions

u(i)¡x+ j ¢ = gi j(u (xj)) , i = 0, ..., n − 1, (3) where gi

j, for j = 1, ..., m,are given real valued functions satisfying some adequate conditions, and xj ∈ (0, 1) , such that 0 = x0< x1< ... < xm< xm+1= 1.

The arguments applied in this paper make use of the lower and upper solu-tion method combined with an iterative technique (suggested in [1]) which is not necessarily monotone, together with classical results such as Lebesgue Dominated Convergence Theorem, Ascoli-Arz`ela Theorem and fixed point theory.

An example is presented to illustrate the existence and location part of the lower and upper solution method.

2. Definitions and auxiliary results. In this section some notations, definitions and auxiliary results, needed for the main existence result, are presented. For

m ∈ N, let 0 = x0 < x1 < ... < xm < xm+1 = 1, D = {x1, ..., xm} and define

j := lim

x→x±j x, for j = 1, ..., m.

Consider P C(s)(I) , s = 1, ..., n − 1, as the space of the real-valued functions u, such that u(s) ∈ P C (I) , u(s)¡x+

k ¢ and u(s)¡x k ¢ exist with u(s)¡x k ¢ = u(s)(x k) , for k = 1, 2, ..., m. Therefore u ∈ P Cn−1(I) , it can be written as

u (x) =          u0(x) if x ∈ [0, x1] , u1(x) if x ∈ (x1, x2] , .. . um(x) if x ∈ (xm, 1] , where um(x) ∈ Cn−1((xi, xi+1)) for i = 1, ..., m.

Denote

P CDn−1(I) = n

u ∈ P Cn−1(I) : u(n−1)∈ AC (xi, xi+1) , i = 0, 1, ..., m o and for each u ∈ P Cn−1

D (I) we set the norm

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where

kwk = sup

x∈I|w (x)| .

Throughout this paper the following hypothesis will be assumed:

(I1) f : [0, 1] × Rn → R is a L1-Carath´eodory function, that is, f (x, ·, ..., ·) is a continuous function for a.e. x ∈ I; f (·, y0, ..., yn−1) is measurable for (y0, ..., yn−1) ∈ Rn; and for every M > 0 there is a real-valued function

ψM ∈ L1([0, 1]) such that

|f (y0, ..., yn−1)| ≤ ψM(x) , for a. e. x ∈ [0, 1]

and for every (y0, ..., yn−1) ∈ Rn with |yi| ≤ M , for i = 0, ..., n − 1. (I2) the real valued functions gi

jare nondecreasing, for j = 1, ..., m and i = 0, ..., n− 1.

Definition 2.1. A function u ∈ P CDn−1(I) is a solution of (1)-(3) if it satisfies (1) almost everywhere in I \ D, the periodic conditions (2) and the impulse conditions (3).

Next Lemma is a key tool to obtain the main result .

Lemma 2.2. Let p : [0, 1] × R → R be a L1−Carath´eodory function such that (v − w) [p (x, v) − p (x, w)] ≤ 0, ∀x ∈ [0, 1] , ∀v, w ∈ R. (4)

Then for each ai

j ∈ R, for j = 1, ..., m, and i = 0, ..., n − 1, the initial value problem

composed by the equation

u(n)(x) = p³x, u(n−1)(x)´ for a. e. x ∈ (0, 1) (5)

and the boundary conditions u(i)¡x+

j ¢

= ai

j, for i = 0, ..., n − 1, (6)

has a unique solution u ∈ P CDn−1(I) .

Proof. The solution of (5)-(6) can be written as

u (x) := n−1 X i=0 ai j ¡ x − x+ j ¢i i! + x Z x+ j (x − r)n−1 (n − 1)! u (n)(r) dr. (7)

As p¡x, u(n−1)(x)¢is bounded in I × R, we can define N :=°°p¡x, u(n−1)(x)¢°° 1, where || · ||1 is the usual norm in L1(I × R), and the following estimates can be obtained for x ∈ (xj, xj+1) |u (x)| ≤n−1P i=0 |ai j| i! + N, |u0(x)| ≤n−1P i=1 |ai j| (i−1)!+ N, .. . ¯ ¯u(n−1)(x)¯¯ ≤¯¯an−1 j ¯ ¯ + N

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Hence, as n is finite, for δ :=n−1P i=0 |ai j| i! +...+ n−1P i=1 |ai j| (i−1)!+ ¯ ¯an−1 j ¯ ¯+nN, it is obtained that kukD= n−1X i=0 ° ° °u(i) ° ° ° = kuk + ku0k + ... + ° ° °u(n−1) ° ° ° ≤ δ. (8)

Let u ∈ P CDn−1(I) be such that kukD≤ δ.

Define the operator T : P CDn−1(I) → P CDn−1(I) given by

T u := n−1X i=0 ai j ¡ x − x+ j ¢i i! + x Z x+ j (x − r)n−1 (n − 1)! u (n)(r) dr (9)

As p¡x, u(n−1)(x)¢is a L1−Carath´eodory function, then T is continuous and, by (8), kT unkD= kT unk + ° °(T un)0 ° ° + ... +°°°(T un)(n−1) ° ° ° ≤ δ.

Moreover the operator T is uniformly bounded and equicontinuous, therefore, by Ascoli-Arzela’s theorem, T is a compact operator. As the set of solutions of the equation u = T u is bounded, then using Schauder fixed point theorem, T has a fixed point u ∈ P CDn−1(I) which satisfies (7) and

u(i)¡x+ j

¢ = ai

j, for i = 0, ..., n − 1. which proves the existence of solution for problem (5)-(6).

To show uniqueness, we assume that the problem (5)-(6) has two solutions, u1 and u2, define z(x) = u(n−1)1 (x) − u(n−1)2 (x) for x ∈]xj, xj+1].

By (4), we have for x ∈]xj, xj+1] z(x) z0(x) =hu(n−1) 1 (x) − u (n−1) 2 (x) i h p(x, u(n−1)1 (x)) − p(x, u(n−1)2 (x)) i ≤ 0.

On the other hand as z¡x+ j ¢ = 0 Z x x+j z(t) z0(t)dt = (z(x)) 2 2 ¡ z(x+ j) ¢2 2 ≥ 0.

So z (x) = 0, for every x ∈]xj, xj+1], and, by integration and (6), u(n−1)1 (x) =

u(n−1)2 (x) for x ∈]xj, xj+1].

Lower and upper functions will be given by the next definition:

Definition 2.3. A function α ∈ P Cn−1

D (I) is said to be a lower solution of the problem (1)-(3) if:

(i) α(n)(x) ≤ f¡x, α (x) , ..., α(n−1)(x)¢, for a.e. x ∈ (0, 1) ,

(ii) α(i)(0) ≤ α(i)(1) , i = 0, ..., n − 1,

(iii) α(i)¡x+ j ¢ ≤ gi j(α (xj)) , for i = 0, ..., n − 1. A function β ∈ P Cn−1

D (I) is said to be a upper solution of the problem (1)-(3) if the reversed inequalities hold.

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3. Existence of solutions. In this section the main existence and location result is presented.

Theorem 3.1. Let α, β be, respectively, lower and upper solutions of (1)-(3) such that

α(n−1)(x) ≤ β(n−1)(x) on I\ D, (10)

and

α(i)(0) ≤ β(i)(0) , i = 0, ..., n − 2. (11)

Assume that conditions (I1) and (I2) hold and f ³ x, α, ..., α(n−2), yn−1 ´ ≤ f (x, y0, .., yn−2, yn−1) ≤ f ³ x, β, ..., β(n−2), yn−1 ´ , (12)

for fixed (x, yn−1) ∈ I × R , α(i)(x) ≤ yi≤ β(i)(x) , for i = 0, ..., n − 2.

Also, for x ∈ [0, 1], α(i)(x) ≤ y

i≤ β(i)(x) , for i = 0, ..., n − 2 and for v, w ∈ R, (v − w) [f (x, y0, y1, .., yn−2, v) − f (x, y0, y1, .., yn−2, w)] ≤ 0.

Then the problem (1)-(3) has a solution u (x) ∈ P CDn−1(I), such that

α(i)(x) ≤ u(i)(x) ≤ β(i)(x) , for i = 0, ..., n − 1

for x ∈ I\D.

Remark 1. As one can notice by (11) the inequalities α(i)(x) ≤ β(i)(x) hold for i = 0, ..., n − 2 and every x ∈ I.

Proof. Consider the following modified problem composed by the equation

u(n)(x) = f³x, δ 0(x, u (x)) , ..., δn−1 ³ x, u(n−1)(x)´´ (13) −u(n−1)(x) + δn−1 ³ x, u(n−1)(x) ´ ,

for x ∈ (0, 1) and x 6= xj where the continuous functions δi : R2 → R, for i = 0, ..., n − 1, are given by δi(x, yi) =    β(i)(x) , y i> β(i)(x) yi , α(i)(x) ≤ yi≤ β(i)(x) α(i)(x) , y i< α(i)(x) , (14) with the boundary conditions (2) and the impulse assumptions (3).

To prove the existence of solution for the problem (13),(2),(3) we apply an iter-ative method, which is not necessarily monotone. Let (ul)l∈N be the sequence of function in P CDn−1(I) defined as follows

u0= α (15) and for l = 1, 2, ... u(n)l (x) = f ³ x, δ0(x, ul−1(x)) , ..., δn−2 ³ x, u(n−2)l−1 (x) ´ , δn−1 ³ x, u(n−1)l (x) ´´ −u(n−1)l (x) + δn−1 ³ x, u(n−1)l (x) ´ , (16) for a.e. x ∈ (0, 1) with the boundary conditions

u(i)l (0) = u(i)l−1(1) , i = 0, ..., n − 1 (17) and the impulsive conditions, for j = 1, ..., m,

u(i)l ¡x+j¢= gi

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By Lemma2.2the sequence (ul)l∈N is well defined.

Step 1 - Every solution of (16)-(18) verifies

α(i)(x) ≤ u(i)l (x) ≤ β(i)(x) , for i = 0, ..., n − 1, (19)

for all l ∈ N and every x ∈ I.

Let u be a solution of the problem (16)-(18). The proof of the inequalities (19) will be done using mathematical induction.

For i = n − 1, consider the inequalities

α(n−1)(x) ≤ u(n−1)l (x) ≤ β(n−1)(x) . For l = 0 , by (15) α(n−1)(x) = u(n−1) 0 (x) ≤ β(n−1)(x) , for x ∈ I\D, and by Remark1 α(i)(x) = u(i) 0 (x) ≤ β(i)(x) , for i = 0, ..., n − 2. Suppose that for k = 1, ..., n − 1, for x ∈ I,

α(n−1)(x) ≤ u(n−1)k (x) ≤ β(n−1)(x) . (20) For x = 0, by (17), (20) and Definition2.3,

u(n−1)l (0) = u(n−1)l−1 (1) ≥ α(n−1)(1) ≥ α(n−1)(0) . If x = x+j, j = 1, ..., m, from (18), (I2), (20) and Definition2.3,

u(n−1)l ¡x+ j ¢ = gn−1 j ³ u(n−1)l−1 (xj) ´ ≥ gn−1 j ³ α(n−1)(x j) ´ ≥ α(n−1)¡x+ j ¢ .

For x ∈ ]xj, xj+1] , j = 1, 2, ..., m, suppose, by contradiction, that there exists

x∗∈ ]x

j, xj+1] such that α(n−1)(x∗) > u(n−1)l (x∗) and define min x∈]xj,xj+1] u(n−1)l (x) − α(n−1)(x) := u(n−1) l (x∗) − α(n−1)(x∗) < 0. As by (18), u(n−1)l ¡x+j¢≥ α(n−1)¡x+ j ¢

, then there is an interval (x, x) ⊂ (xj, x∗) such that

u(n−1)l (x) < α(n−1)(x) and u(n)

l (x) ≤ α(n)(x) , ∀x ∈ (x, x) . From (13) and (12) the following contradiction is obtained for x ∈ (x, x)

0 ≥ u(l)l (x) − α(n)(x) = f³x, δ0(x, ul−1(x)) , ..., δn−2 ³ x, u(n−2)l−1 (x)´, α(n−1)(x)´ −u(n−1)(x) + α(n−1)(x) − α(n)(x) ≥ f ³ x, α (x) , ..., α(n−1)(x)´− u(n−1)(x) + α(n−1)(x) −f ³ x, α (x) , ..., α(n−1)(x) ´ ≥ α(n−1)(x) − u(n−1)(x) > 0.

Therefore u(n−1)l (x) ≥ α(n−1)(x) , for all l ∈ N and every x ∈ I. In the same way it can be shown that u(n−1)l (x) ≤ β(n−1)(x) , ∀x ∈ I, ∀l ∈ N, and so (19) is proved when i = n − 1.

Consider now the inequality α(n−2)(x) ≤ u(n−2)

l (x) ≤ β(n−2)(x) , for all l ∈ N and every x ∈ I.

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To justify (19) for i = n − 2, notice that for n = 0, the proof is obtained in a similar way as in above.

Assuming that for l = 1, ..., n − 1 and every x ∈ I,

α(n−2)(x) ≤ u(n−2)

l (x) ≤ β(n−2)(x) . (21)

then for x ∈ [0, x1], by integration of the inequality u(n−1)l (x) ≥ α(n−1)(x) in [0, x] we have

u(n−2)l (x) − u(n−2)l (0) ≥ α(n−2)(x) − α(n−2)(0) . By (17) and (21),

u(n−2)l (x) ≥ α(n−2)(x) − α(n−2)(0) + u(n−2)l−1 (1)

≥ α(n−2)(x) − α(n−2)(0) + α(n−2)(1) ≥ α(n−2)(x) hence u(n−2)l (x) ≥ α(n−2)(x) , for all x ∈ [0, x1] .

For x ∈ ]xj, xj+1] , j = 1, 2, ..., m, by integration of the inequality u(n−1)l (x) ≥

α(n−1)(x) in x ∈ ]x j, xj+1], u(n−2)l (x) ≥ α(n−2)(x) − α(n−2)¡x+ j ¢ + u(n−2)l ¡x+ j ¢ ,

and by (18) and Definition2.3

u(n−2)l (x) ≥ α(n−2)(x) − α(n−2)¡x+ j ¢ + gn−2 j ³ u(n−2)l−1 (xj) ´ ≥ α(n−2)(x) . obtaining that u(n−2)l (x) ≥ α(n−2)(x) , for all l ∈ N and every x ∈ I. Using similar arguments it can be proved that u(n−2)l (x) ≤ β(n−2)(x) and therefore

α(n−2)(x) ≤ u(n−2)

l (x) ≤ β(n−2)(x) , ∀x ∈ I, ∀l ∈ N. (22) The remaining inequalities in (19) can be proved as in above, by integration of (21) in [0, x1], applying the correspondent induction hypothesis as well as conditions (17), (18) and Definition 2.3.

Step 2 - The sequence (ul)l∈N is convergent to u solution of (16)-(18). Let Ci = max

©°

°α(i)°° ,°°β(i)°°ª, for i = 0, ..., n − 1, so there exists M > 0, with

M :=Pn−1i=0 Ci, and for all l ∈ N,

kulkD≤ M. (23)

Let Ω be a compact subset of Rn given by

Ω = {(w0, ..., wn−1) ∈ Rn : kwik ≤ Ci, i = 0, ..., n − 1} .

As f is a L1-Carath´eodory function in Ω, then there exists a real-valued function

ψM(x) ∈ L1(I), such that

|f (x, w0, ..., wn−1)| ≤ ψM(x) , for every (w0, ..., wn−1) ∈ Ω. (24) By Step1 and (23), ³ ul, u0l, ..., u (n−1) l ´

∈ Ω, for all l ∈ N. From (16) and (24) we

obtain ¯ ¯ ¯u(n)l (x) ¯ ¯ ¯ ≤ ψM(x) + 2Cn−1, for a.e. x ∈ I, hence u(n)l (x) ∈ L1(I) .

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By integration in I we obtain that u(n−1)l (x) = u(n−1)l (0) + Z x 0 u(n)l (s) ds + X 0<xj≤x gjn−1 ³ u(n−1)l−1 (xj) ´ ,

therefore u(n−1)l ∈ AC (xj, xj+1) and ul ∈ P CDn−1(I) . By Ascoli-Arz`ela Theorem there exists a subsequence denoted by (ul)l∈N, which converges to u ∈ P CDn−1(I) . Then¡u, u0, ..., u(n−1)¢∈ Ω.

Using the Lebesgue dominated convergence theorem, for x ∈ (xj, xj+1) , Z x xj   f ³ s, δ0(s, ul−1(s)) , ..., δn−2 ³ s, u(n−2)l−1 (s)´, δn−1 ³ s, u(n−1)l (s)´´ −u(n−1)l (x) + δn−1 ³ x, u(n−1)l (x)´   ds is convergent to Z x xj · f¡s, δ0(s, u (s)) , ..., δn−2 ¡ s, u(n−2)(s)¢, δ n−1 ¡ s, u(n−1)(s)¢¢ −u(n−1)(s) + δ n−1 ¡ s, u(n−1)(s)¢ ¸ ds as l → ∞. Therefore as l → ∞ u(n−1)l (x) = u(n−1)l (xj) + Z x xj   f ³ s, δ0(s, ul−1(s)) , ..., δn−2 ³ s, u(n−2)l−1 (s)´, δn−1 ³ s, u(n−1)l (s)´´ −u(n−1)l (x) + δn−1 ³ x, u(n−1)l (x) ´   ds is convergent to u(n−1)(x) = u(n−1)(xj) + Z x xj · f¡s, δ0(s, u (s)) , ..., δn−2 ¡ s, u(n−2)(s)¢, δ n−1 ¡ s, u(n−1)(s)¢¢ −u(n−1)(s) + δ n−1 ¡ s, u(n−1)(s)¢ ¸ ds.

As the function f is L1-Carath´eodory function in (x

j, xj+1), then u(n−1)(x) ∈

AC (xj, xj+1) . Therefore u ∈ P CDn−1(I) and u is a solution of (16)-(18).

To prove that u is a solution of the initial problem (1)-(3) we note that taking the limit in (17) and (18), as l → ∞, by the convergence of ul then u verifies (2) and, by the continuity of the impulsive functions, u verifies (3). By (14), Step 1 and the convergence of ul, u verifies (1).

Then problem (1)-(3) has a solution u (x) ∈ P CDn−1(I), such that

α(i)(x) ≤ u(i)(x) ≤ β(i)(x) , for i = 0, ..., n − 1, for x ∈ I.

4. Example. Let us consider the fifth order nonlinear impulsive boundary value problem, composed by the equation

u(v)(x) = u (x) + u0(x) − u00(x) + (u000(x) + 1)3 + k ¯ ¯ ¯u(iv)(x) ¯ ¯ ¯θ (25)

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where 0 < θ ≤ 2 and k ≤ −32, for all x ∈ [0, 1] \ ©1 2 ª

along with the boundary conditions (2) and for x = 1

2 the impulse conditions

u³1 2 +´ = µ1¡u¡1 2 ¢¢ u0³1 2 +´ = µ2¡u0¡1 2 ¢¢1 2 u00³1 2 +´ = µ3¡u00¡1 2 ¢¢3 u000³1 2 +´ = µ4¡u000¡1 2 ¢¢5 u(iv)³1 2 +´ = µ5¡u(iv)¡1 2 ¢¢1 3 (26) with µi∈ R+, i = 1, 2, 3, 4.

Obviously this problem is a particular case of (1)-(3) with

f (x, y0, y1, y2, y3, y4) = y0+ y1− y2+ (y3+ 1)3+ k |y4|θ, for all x ∈ [0, 1] \ ©1

2 ª

, m = 1, x1 = 12 and the nondecreasing functions g1i,

i = 0, 1, 2, 3, 4 given by g0 1(x) = µ1x, g11(x) = µ2x 1 2, g12(x) = µ3x3, g13(x) = µ4x5, g41(x) = µ5x 1 3.

One can verify that the functions α (x) = 0 and

β (x) = ( x4 24 +x 3 6 +x 2 2 + x + 1 , x ∈ £ 0,1 2 ¤ x4 24 , x ∈ ¡1 2, 1 ¤ are P C4 D(I) for D = ©1 2 ª and considering β0(x) = ( x3 6 +x 2 2 + x + 1 , x ∈ £ 0,1 2 ¤ x3 6 , x ∈ ¡1 2, 1 ¤ , β00(x) = ( x2 2 + x + 1 , x ∈ £ 0,1 2 ¤ x2 2 , x ∈ ¡1 2, 1 ¤ and β000(x) = ½ x + 1 , x ∈£0,1 2 ¤ x , x ∈¡1 2, 1 ¤ ,

they are lower and upper solutions, respectively, for the problem (25), (2), (26), with 0 ≤ µ1≤ 1 633, µ2 237 948 , µ3 64 2197, µ4 1 64, µ5≤ 1. As f verifies (12), therefore by Theorem 3.1there is a solution u (x) ∈ P C4

D(I), such that, α(i)(x) ≤ u(i)(x) ≤ β(i)(x) , for i = 0, 1, 2, 3, 4.

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[6] R. Liang, J. Shen, Periodic boundary value problem for the first order impulsive functional differential equations. J. Comput. Appl. Math. 202 (2007) 498–510.

[7] Z. Luo, Z. Jing, Periodic boundary value problem for first-order impulsive functional differ-ential equations. Comput. Math. Appl. 55 (2008) 2094–2107.

[8] I. Rach˚unkov´a, M. Tvrd´y, Existence results for impulsive second-order periodic problems. Nonlinear Anal. 59 (2004) 133–146.

[9] X. Wang, J. Zhang, Impulsive anti-periodic boundary value problem of first-order integro-differential equations. J. Comput. Appl. Math. 234 (2010) 3261-3267.

[10] H. Wu, Y. Liu, Periodic boundary value problems of fourth order impulsive differential equa-tions, 2011 International Symposium on IT in Medicine and Education (ITME), Volume: 2 (2011) 424 - 427.

[11] G. Ye, X. Zhou, L. Huang, Periodic Boundary Value Problems for Nonlinear Impulsive Dif-ferential Equations of Mixed Type, Intelligent System Design and Engineering Application (ISDEA), (2012) 452 - 455.

Received xxxx 20xx; revised xxxx 20xx. E-mail address: jfzero@gmail.com

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