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Existence of Solutions for a Weighted -Laplacian Impulsive Integrodifferential System with Multipoint and Integral Boundary Value Conditions

Abstract

By the Leray-Schauder's degree, the existence of solutions for a weighted -Laplacian impulsive integro-differential system with multi-point and integral boundary value conditions is considered. The sufficient results for the existence are given under the resonance and nonresonance cases, respectively. Moreover, we get the existence of nonnegative solutions at nonresonance.

1. Introduction

In this paper, we consider the existence of solutions for the following weighted -Laplacian integrodifferential system:

(1.1)

where , , , , with the following impulsive boundary value conditions

(1.2)
(1.3)
(1.4)

where and , is called the weighted -Laplacian; , ; , and ; is nonnegative, with ; ; and are linear operators defined by , , , where .

If and , we say the problem is nonresonant, but if and , we say the problem is resonant.

Throughout the paper, means function which uniformly convergent to 0 (as ); for any , will denote the th component of ; the inner product in will be denoted by ; will denote the absolute value and the Euclidean norm on . Denote , , , , , where , . Denote the interior of , . Let

(1.5)

satisfies , for all , and ;

(1.6)

For any , denote . Obviously, is a Banach space with the norm , and is a Banach space with the norm . Denote with the norm , for all , where .

For simplicity, we denote and by and , respectively, and denote

(1.7)

In recent years, there has been an increasing interest in the study of differential equations with nonstandard -growth conditions. These problems have many interesting applications (see [14]). Many results have been obtained on these kinds of problems, for example [517]. If (a constant), (1.1)–(1.4) becomes the well known -Laplacian problem. If is a general function, one can see easily that in general, while , so represents a non-homogeneity and possesses more nonlinearity, thus is more complicated than . For example, we have the following.

(a)In general, the infimum of eigenvalues for the -Laplacian Dirichlet problems is zero, and only under some special conditions (see [10]). When () is an interval, the results in [10] show that if and only if is monotone. But the property of is very important in the study of -Laplacian problems, for example, in [18], the authors use this property to deal with the existence of solutions.

(b)If and (a constant) and , then is concave, this property is used extensively in the study of one-dimensional -Laplacian problems (see [19]), but it is invalid for . It is another difference between and .

Recently, there are many works devoted to the existence of solutions to the Laplacian impulsive differential equation boundary value problems, for example [2028]. Many methods had been applied to deal with these problems, for example sub-super-solution method, fixed point theorem, monotone iterative method, coincidence degree, variational principles (see [29]), and so forth. Because of the nonlinearity of , results about the existence of solutions for -Laplacian impulsive differential equation boundary value problems are rare (see [30]). In [31], using coincidence degree method, the present author investigate the existence of solutions for -Laplacian impulsive differential equation with multipoint boundary value conditions. Integral boundary conditions for evolution problems have various applications in chemical engineering, thermoelasticity, underground water flow and population dynamics, there are many papers on the differential equations with integral boundary value problems, for example, [3235].

In this paper, when is a general function, we investigate the existence of solutions and nonnegative solutions for the weighted -Laplacian impulsive integrodifferential system with multipoint and integral boundary value conditions. Our results contain both the cases of resonance and nonresonance, and the method is based upon Leray-Schauder's degree. Moreover, this paper will consider the existence of (1.1) with (1.2), (1.4) and the following impulsive condition:

(1.8)

where , the impulsive condition (1.8) is called linear impulsive condition (LI for short), and (1.3) is called nonlinear impulsive condition (NLI for short). In generaly, -Laplacian impulsive problems have two kinds of impulsive conditions, that is, LI and NLI.

Let , the function is assumed to be Caratheodory, by this we mean the following:

(i)for almost every the function is continuous;

(ii)for each the function is measurable on ;

(iii)for each there is a such that, for almost every and every with , , , , one has

(1.9)

We say a function is a solution of (1.1) if with absolutely continuous on , , which satisfies (1.1) a.e. on .

In this paper, we always use to denote positive constants, if it cannot lead to confusion. Denote

(1.10)

We say satisfies sub- growth condition, if satisfies

(1.11)

where , and .

This paper is organized as four sections. In Section 2, we present some preliminary and give the operator equation which has the same solutions of (1.1)–(1.4). In Section 3, we give the existence of solutions and nonnegative solutions for system (1.1)–(1.4) at nonresonance. Finally, in Section 4, we give the existence of solutions for system (1.1)–(1.4) at resonance.

2. Preliminary

For any , denote . Obviously, has the following properties.

Lemma 2.1 (see [31]).

is a continuous function and satisfies the following.

(i)For any , is strictly monotone, satisfying

(2.1)

(ii)There exists a function , as , such that

(2.2)

It is well known that is an homeomorphism from to for any fixed . Denote

(2.3)

It is clear that is continuous and sends bounded sets to bounded sets.

In this section, we will do some preparation and give the operator equation which has the same solutions of (1.1)–(1.4). At first, let us now consider the following simple impulsive problem with boundary value condition  (1.4)

(2.4)

where ; .

We will discuss (2.4) with (1.4) in the cases of resonance and nonresonance, respectively.

2.1. The Case of Nonresonance

Suppose and . If is a solution of (2.4) with (1.4), we have

(2.5)

Denote , , . It is easy to see that is dependent on and . Define operator as

(2.6)

By solving for in (2.5) and integrating, we find

(2.7)

which together with the boundary value condition (1.4) implies

(2.8)

Denote with the norm , for all , then is a Banach space.

We define as

(2.9)

then is continuous. Throughout the paper, we denote . It is easy to see the following.

Lemma 2.2.

The function is continuous and sends bounded sets to bounded sets. Moreover, for any , we have

(2.10)

We denote the Nemytskii operator associated to defined by

(2.11)

We define as

(2.12)

where , .

It is clear that is continuous and sends bounded sets of to bounded sets of , and hence it is compact continuous.

If is a solution of (2.4) with (1.4), we have

(2.13)

For fixed , we define as

(2.14)

Define as

(2.15)

Lemma 2.3.

  1. (i)

    The operator is continuous and sends equiintegrable sets in to relatively compact sets in .

  2. (ii)

    The operator is continuous and sends bounded sets in to relatively compact sets in .

Proof.

(i)   It is easy to check that , for all , for all . Since and

(2.16)

it is easy to check that is a continuous operator from to .

Let be an equiintegrable set in , then there exists , such that

(2.17)

We want to show that is a compact set.

Let be a sequence in , then there exists a sequence such that . For any , we have

(2.18)

Hence the sequence is uniformly bounded and equicontinuous. By Ascoli-Arzela theorem, there exists a subsequence of (which we rename the same) which is convergent in . According to the bounded continuous of the operator , we can choose a subsequence of (which we still denote by ) which is convergent in , then is convergent in .

Since

(2.19)

it follows from the continuity of and the integrability of in that is convergent in . Thus is convergent in .

  1. (ii)

    It is easy to see from (i) and Lemma 2.2.

This completes the proof.

Let us define as .

It is easy to see that is compact continuous.

Lemma 2.4.

Suppose and , then is a solution of (1.1)–(1.4) if and only if is a solution of the following abstract operator equation

(2.20)

Proof.

Suppose is a solution of (1.1)–(1.4). From the definition of and , similar to the discussion before Lemma 2.2, we know that is a solution of (2.20).

Conversely, if is a solution of (2.20), then (1.2) is satisfied.

From (2.20), we have

(2.21)

It follows from (2.21) that (1.3) is satisfied.

From (2.21) and the definition of , we have

(2.22)

From (2.20) and the definition of , it is easy to check that

(2.23)

It follows from (2.22) and (2.23) that (1.4) is satisfied.

Hence is a solutions of (1.1)–(1.4). This completes the proof.

2.2. The Case of Resonance

Suppose and . If is a solution of (2.4) with (1.4), we have

(2.24)

Denote , , . It is easy to see that is dependent on and .

The boundary value condition (1.4) implies that

(2.25)

For any , we denote

(2.26)

Lemma 2.5.

The function has the following properties.

(i)For any fixed , the equation

(2.27)

has unique solution .

(ii)The function , defined in (i), is continuous and sends bounded sets to bounded sets. Moreover, for any , we have

(2.28)

where

(2.29)

Proof.

  1. (i)

    From Lemma 2.1, it is immediate that

    (2.30)

and hence, if (2.27) has a solution, then it is unique.

Set

(2.31)

Suppose , it is easy to see that there exists some such that, the absolute value of the th component of satisfies

(2.32)

Thus the th component of keeps sign on , then it is not hard to check that the th component of keeps the same sign of .

Thus . Let us consider the equation

(2.33)

According to the preceding discussion, all the solutions of (2.33) belong to . Therefore

(2.34)

it means the existence of solutions of .

In this way, we define a function , which satisfies .

  1. (ii)

    By the proof of (i), we also obtain sends bounded sets to bounded sets, and

    (2.35)

It only remains to prove the continuity of . Let is a convergent sequence in and , as . Since is a bounded sequence, it contains a convergent subsequence . Suppose as . Since , letting , we have , which together with (i) implies , it means is continuous. This completes the proof.

We define as

(2.36)

where , .

It is clear that is continuous and sends bounded sets of to bounded sets of , and hence it is a compact continuous mapping.

Let us define

(2.37)

and as

(2.38)

Similar to the proof of Lemma 2.3, we have the following lemma.

Lemma 2.6.

The operator is continuous and sends equiintegrable sets in to relatively  compact sets in .

Denote

(2.39)

Lemma 2.7.

Suppose and , then is a solution of (1.1)–(1.4) if and only if is a solution of the following abstract operator equation

(2.40)

Proof.

Suppose is a solution of (1.1)–(1.4), it is clear that is a solution of (2.40).

Conversely, if is a solution of (2.40), then (1.2) is satisfied and

(2.41)

Thus .

From (2.40) and (2.41), we have

(2.42)

According to (2.42), we get that (1.3) is satisfied. Since , we have

(2.43)

It follows from the definition of that

(2.44)

then .

Hence is a solutions of (1.1)–(1.4). This completes the proof.

3. Existence of Solutions in the Case of Nonresonance

In this section, we will apply Leray-Schauder's degree to deal with the existence of solutions and nonnegative solutions for system (1.1)–(1.4) at nonresonance.

When satisfies sub- growth condition, we have the following.

Theorem 3.1.

Suppose and , satisfies sub- growth condition, and operators and satisfy the following condition

(3.1)

then problem (1.1)−(1.4) has at least one solution.

Proof.

First we consider the following problem:

(S1)

Denote

(3.2)

where is defined in (2.11).

We know that (S1) has the same solution of the following operator equation when ,

(3.3)

It is easy to see that operator is compact continuous for any . It follows from Lemmas 2.2 and 2.3 that is compact continuous from to for any .

We claim that all the solutions of (3.3) are uniformly bounded for . In fact, if it is false, we can find a sequence of solutions for (3.3) such that as , and for any .

From Lemma 2.2, we have

(3.4)

Thus

(3.5)

From (S1), we have

(3.6)

It follows from (2.12) and Lemma 2.2 that

(3.7)

Denote . The above inequality holds

(3.8)

It follows from (3.1) and (3.5) that

(3.9)

For any , we have

(3.10)

which implies that , ; . Thus

(3.11)

It follows from (3.8) and (3.11) that is uniformly bounded.

Thus, we can choose a large enough such that all the solutions of (3.3) belong to . Therefore the Leray-Schauder degree is well defined for , and

(3.12)

It is easy to see that is a solution of if and only if is a solution of the following usual differential equation

(S2)

Obviously, system (S2) possesses a unique solution . Since , we have

(3.13)

which implies that (1.1)–(1.4) has at least one solution. This completes the proof.

Theorem 3.2.

Suppose and , satisfies sub- growth condition, and operators and satisfy the following

(3.14)

where , and , , then problem (1.1) with (1.2), (1.4), and (1.8) has at least one solution.

Proof.

Obviously,

(3.15)

From Theorem 3.1, it suffices to show that

(3.16)

(a)Suppose , where is a large enough positive constant. From the definition of , we have

(3.17)

Since , we have . Thus (3.16) is valid.

(b)Suppose , we have

(3.18)

There are two cases.

Case 1 ().

Since , we have , and then

(3.19)

Thus (3.16) is valid.

Case 2 ().

Since , we have , and

(3.20)

Thus (3.16) is valid. Thus problem (1.1) with (1.2), (1.4), and (1.8) has at least one solution. This completes the proof.

Let us consider

(3.21)

where is a parameter, and

(3.22)

where , are Caratheodory.

We have the following.

Theorem 3.3.

Suppose and , satisfies sub- growth condition, and we assumethat

(3.23)

then problem (3.21) with (1.2)–(1.4) has at least one solution when the parameter is small enough.

Proof.

Denote

(3.24)

We consider the existence of solutions of the following equation with (1.2)–(1.4)

(3.25)

Denote

(3.26)

where is defined in (2.11).

We know that (3.25) with (1.2)–(1.4) has the same solution of .

Obviously, . So . As in the proof of Theorem 3.1, we know that all the solutions of are uniformly bounded, then there exists a large enough such that all the solutions of belong to . Since is compact continuous from to , we have

(3.27)

Since are Caratheodory, we have

(3.28)

Thus

(3.29)

Obviously, . We obtain

(3.30)

Thus, when is small enough, we can conclude that

(3.31)

Thus has no solution on for any , when is small enough. It means that the Leray-Schauder degree is well defined for any , and

(3.32)

Since , from the proof of Theorem 3.1, we can see that the right hand side is nonzero. Thus (3.21) with (1.2)–(1.4) has at least one solution. This completes the proof.

Theorem 3.4.

Suppose and , satisfies sub- growth condition, and we assumethat

(3.33)

where , and , , then problem (3.21) with (1.2), (1.4), and (1.8) has at least one solution when the parameter is small enough.

Proof.

As it is similar to the proof of Theorems 3.2 and 3.3, we omit it here.

In the following, we will consider the existence of nonnegative solutions. For any , the notation means for any .

Theorem 3.5.

Suppose , , we also assume

, for all;

for any , , for all .

Then every solution of (1.1)–(1.4) is nonnegative.

Proof.

Let be a solution of (1.1)–(1.4), integrating (1.1) from 0 to , we have

(3.34)

where . The boundary value condition holds

(3.35)

Conditions (10)-(20) mean . Obviously, for any for all , we have

(3.36)

It follows from conditions (10)-(20) and (3.36) that is increasing on , namely , for all with . Thus the boundary value condition holds , then .

Since is increasing and , we have , for all .

Thus every solution of (1.1)–(1.4) is nonnegative. The proof is completed.

Corollary 3.6.

Under the conditions of Theorem 3.1, we also assume

, for all with ;

for any , , for all with ;

for any and , , .

Then (1.1)–(1.4) has a nonnegative solution.

Proof.

Define , where

(3.37)

Denote

(3.38)

then satisfies Caratheodory condition, and for any .

For any , we denote

(3.39)

then and are continuous, and satisfy

(3.40)

It is not hard to check that

, for uniformly, where , and ;

, for all ;

, for all .

Let us consider

(3.41)

It follows from Theorems 3.1 and 3.5 that (3.41) have a nonnegative solution . Since , we have . Thus is a nonnegative solution of (1.1)−(1.4). This completes the proof.

4. Existence of Solutions in the Case of Resonance

In the following, we will consider the existence of solutions for system (1.1)–(1.4) at resonance.

Theorem 4.1.

Suppose and , is an open bounded set in such that the following conditions hold.

For each the problem

(4.1)

has no solution on .

The equation

(4.2)

has no solution on .

The Brouwer degree .

Then problem (1.1)–(1.4) have a solution on .

Proof.

Let us consider the following impulsive equation

(4.3)

For any , if is a solution to (4.1) or is a solution to (4.3), we have necessarily

(4.4)

It means that (4.1) and (4.3) have the same solutions for .

We denote defined by

(4.5)

where is defined by (2.11). Denote

(4.6)

Set

(4.7)

then the fixed point of is a solution for (1.1)–(1.4). Also problem (4.3) can be rewritten in the equivalent form

(4.8)

Since is Caratheodory, it is easy to see that is continuous and sends bounded sets into equiintegrable sets. It is easy to see that is compact continuous. From Lemma 2.6, we can conclude that is continuous and compact for any . We assume that (4.8) does not have a solution on for , otherwise we complete the proof. Now from hypothesis (10) it follows that (4.8) has no solutions for . For , (4.3) is equivalent to the following usual problem

(4.9)

If is a solution to this problem, we must have

(4.10)

As this problem is a usual differential equation, we have

(4.11)

where is a constant. Therefore keeps the same sign of . From , we have . From the continuity of , there exist , such that , . Hence , it holds , a constant. Thus (4.10) holds

(4.12)

which together with hypothesis (20) implies that . Thus we have proved that (4.8) has no solution on . Therefore the Leray-Schauder degree is well defined for , and from the homotopy invariant property of that degree we have

(4.13)

Now it is clear that the problem

(4.14)

is equivalent to problem (1.1)–(1.4), and (4.13) tells us that problem (4.14) will have a solution if we can show that

(4.15)

It is not hard to check that . Thus

(4.16)

By the properties of the Leray-Schauder degree, we have

(4.17)

where the function is defined in (4.2) and denotes the Brouwer degree. By hypothesis (30), this last degree is different from zero. This completes the proof.

Our next theorem is a consequence of Theorem 4.1. As an application of Theorem 4.1, let us consider the following system

(4.18)

with (1.2), (1.3), and (1.4), where is Caratheodory, is continuous, and for any fixed , holds , for all , .

Theorem 4.2.

Suppose that the following conditions hold

for all and all , where satisfies ;

, for uniformly;

, for all , where ;

, for all , where ;

for large enough , the equation

(4.19)

has no solution on , where ;

the Brouwer degree for large enough , where .

Then problem (4.18) with (1.2), (1.3), and (1.4) has at least one solution.

Proof.

For any and , we denote

(4.20)

At first, we consider the following problem

(4.21)

As in the proof of Theorem 4.1, we know that (4.21) has the same solutions of

(4.22)

where is defined in (2.39).

We claim that all the solutions of (4.21) are uniformly bounded for . In fact, if it is false, we can find a sequence of solutions for (4.21) such that as , and for any .

Since are solutions of (4.21), we have

(4.23)

.Since , we have

(4.24)

It follows from Lemma 2.5 that

(4.25)

From (30), (40), (4.23) and (4.25), we can see that

(4.26)

From (4.26), we have

(4.27)

Denote , then and . Thus possesses a convergent subsequence (which still denoted by ), then there exists a vector such that and . Without loss of generality, we assume that . Since , there exist such that

(4.28)

Obviously

(4.29)

Note that (as ) and , it follows from (4.27), (4.28), and (30) that

(4.30)

By (4.27), (4.29), and (4.30) we have for uniformly, which implies

(4.31)

where , satisfies , .

From (1.4), we have

(4.32)

Note that , it follows from (4.31), (40) and the continuity of that

(4.33)

which contradicts to (4.32). This implies that there exists a big enough such that all the solutions of (4.21) belong to , then we have

(4.34)

In order to obtaining the existence of solutions (4.18) with (1.2), (1.3), and (1.4), we only need to prove that .

Now we consider the following equation

(4.35)

where .

Similar to the preceding discussion, for any , all the solutions of (4.35) are uniformly bounded.

If is a solution of the following usual equation with (1.4)

(4.36)

we have

(4.37)

As , we have , it means that is a solution of

(4.38)

By hypothesis (50), (4.35) has no solutions on , from Theorem 4.1, we obtain that (4.18) with (1.2), (1.3), and (1.4) has at least one solution. This completes the proof.

Corollary 4.3.

If is Caratheodory, conditions (20), (30) and (40) of Theorem 4.2 are satisfied, condition (30) of Corollary 3.6 is also satisfied, , where are positive functions satisfying ; then (4.18) with (1.2), (1.3), and (1.4) has at least one solution.

Proof.

Denote

(4.39)

From condition (40), we have

(4.40)

Note that and are nonnegative. From the above inequality, we can see that all the solutions of are uniformly bounded for . Thus is well defined for and

(4.41)

and it is easy to see that has a unique solution in and

(4.42)

According to Theorem 4.2, we get that (4.18) with (1.2), (1.3), and (1.4) has at least a solution. This completes the proof.

Let us consider

(4.43)

where is a parameter, and

(4.44)

where are Caratheodory.

From Theorem 4.2, similar to the proof of Theorem 3.3, we have the following.

Theorem 4.4.

If conditions of (10) and (30)–(60) of Theorem 4.2 are satisfied, then problem (4.43) with (1.2), (1.3), and (1.4) has at least one solution when the parameter is small enough.

Theorem 4.5.

If conditions of (10)–(30) and (50)-(60) of Theorem 4.2 are satisfied, and satisfy

(4.45)

where

(4.46)

then problem (4.18) with (1.2), (1.3), and (1.8) has at least one solution.

Proof.

Similar to the proof of Theorem 3.2, the condition (40) of Theorem 4.2 is satisfied. Thus problem (4.18) with (1.2), (1.3) and (1.8) has at least a solution.

Similar to the proof of Theorem 3.2 and Corollary 4.3, we have the following.

Corollary 4.6.

If is Caratheodory, (4.45), (4.46) and conditions (20) and (30) of Theorem 4.2 are satisfied, condition (30) of Corollary 3.6 is also satisfied, , where are positive functions satisfying ; then (4.43) with (1.2), (1.3), and (1.8) has at least one solution when the parameter is small enough.

References

  1. Acerbi E, Mingione G: Regularity results for stationary electro-rheological fluids. Archive for Rational Mechanics and Analysis 2002, 164(3):213–259. 10.1007/s00205-002-0208-7

    Article  MathSciNet  MATH  Google Scholar 

  2. Chen Y, Levine S, Rao M: Variable exponent, linear growth functionals in image restoration. SIAM Journal on Applied Mathematics 2006, 66(4):1383–1406. 10.1137/050624522

    Article  MathSciNet  MATH  Google Scholar 

  3. Růžička M: Electrorheological Fluids: Modeling and Mathematical Theory, Lecture Notes in Mathematics. Volume 1748. Springer, Berlin, Germany; 2000:xvi+176.

    MATH  Google Scholar 

  4. Zhikov VV: Averaging of functionals of the calculus of variations and elasticity theory. Mathematics of the USSR-Izvestiya 1986, 29: 33–36.

    Article  MathSciNet  MATH  Google Scholar 

  5. Acerbi E, Mingione G: Regularity results for a class of functionals with non-standard growth. Archive for Rational Mechanics and Analysis 2001, 156(2):121–140. 10.1007/s002050100117

    Article  MathSciNet  MATH  Google Scholar 

  6. Coscia A, Mingione G: Hölder continuity of the gradient of -harmonic mappings. Comptes Rendus de l'Académie des Sciences. Série I. Mathématique 1999, 328(4):363–368.

    MathSciNet  MATH  Google Scholar 

  7. Deng S-G: A local mountain pass theorem and applications to a double perturbed -Laplacian equations. Applied Mathematics and Computation 2009, 211(1):234–241. 10.1016/j.amc.2009.01.042

    Article  MathSciNet  MATH  Google Scholar 

  8. Fan X: Global regularity for variable exponent elliptic equations in divergence form. Journal of Differential Equations 2007, 235(2):397–417. 10.1016/j.jde.2007.01.008

    Article  MathSciNet  MATH  Google Scholar 

  9. Fan X: Boundary trace embedding theorems for variable exponent Sobolev spaces. Journal of Mathematical Analysis and Applications 2008, 339(2):1395–1412. 10.1016/j.jmaa.2007.08.003

    Article  MathSciNet  MATH  Google Scholar 

  10. Fan X, Zhang Q, Zhao D: Eigenvalues of -Laplacian Dirichlet problem. Journal of Mathematical Analysis and Applications 2005, 302(2):306–317. 10.1016/j.jmaa.2003.11.020

    Article  MathSciNet  MATH  Google Scholar 

  11. Harjulehto P, Hästö P, Latvala V: Harnack's inequality for -harmonic functions with unbounded exponent . Journal of Mathematical Analysis and Applications 2009, 352(1):345–359. 10.1016/j.jmaa.2008.05.090

    Article  MathSciNet  MATH  Google Scholar 

  12. Mihăilescu M, Rădulescu V: Continuous spectrum for a class of nonhomogeneous differential operators. Manuscripta Mathematica 2008, 125(2):157–167. 10.1007/s00229-007-0137-8

    Article  MathSciNet  MATH  Google Scholar 

  13. Mihăilescu M, Pucci P, Rădulescu V: Nonhomogeneous boundary value problems in anisotropic Sobolev spaces. Comptes Rendus de l'Académie des Sciences—Series I 2007, 345(10):561–566.

    MathSciNet  MATH  Google Scholar 

  14. Mihăilescu M, Rădulescu V, Repovš D: On a non-homogeneous eigenvalue problem involving a potential: an Orlicz-Sobolev space setting. Journal de Mathématiques Pures et Appliquées 2010, 93(2):132–148.

    Article  MathSciNet  MATH  Google Scholar 

  15. Musielak J: Orlicz Spaces and Modular Spaces, Lecture Notes in Mathematics. Volume 1034. Springer, Berlin, Germany; 1983:iii+222.

    Google Scholar 

  16. Samko SG: Density in the generalized Sobolev spaces . Doklady Rossiĭskaya Akademiya Nauk 1999, 369(4):451–454.

    MathSciNet  MATH  Google Scholar 

  17. Zhang Q: Existence of solutions for -Laplacian equations with singular coefficients in . Journal of Mathematical Analysis and Applications 2008, 348(1):38–50. 10.1016/j.jmaa.2008.06.026

    Article  MathSciNet  MATH  Google Scholar 

  18. Kim I-S, Kim Yun-Ho: Global bifurcation of the -Laplacian in . Nonlinear Analysis: Theory, Methods & Applications 2009, 70(7):2685–2690. 10.1016/j.na.2008.03.055

    Article  MathSciNet  MATH  Google Scholar 

  19. Ahmad B, Nieto JJ: The monotone iterative technique for three-point second-order integrodifferential boundary value problems with -Laplacian. Boundary Value Problems 2007, -9.

    Google Scholar 

  20. Jiao J, Chen L, Li L: Asymptotic behavior of solutions of second-order nonlinear impulsive differential equations. Journal of Mathematical Analysis and Applications 2008, 337(1):458–463. 10.1016/j.jmaa.2007.04.021

    Article  MathSciNet  MATH  Google Scholar 

  21. Li J, Nieto JJ, Shen J: Impulsive periodic boundary value problems of first-order differential equations. Journal of Mathematical Analysis and Applications 2007, 325(1):226–236. 10.1016/j.jmaa.2005.04.005

    Article  MathSciNet  MATH  Google Scholar 

  22. Liu L, Hu L, Wu Y: Positive solutions of two-point boundary value problems for systems of nonlinear second-order singular and impulsive differential equations. Nonlinear Analysis: Theory, Methods & Applications 2008, 69(11):3774–3789. 10.1016/j.na.2007.10.012

    Article  MathSciNet  MATH  Google Scholar 

  23. Nieto JJ, O'Regan D: Variational approach to impulsive differential equations. Nonlinear Analysis: Real World Applications 2009, 10(2):680–690. 10.1016/j.nonrwa.2007.10.022

    Article  MathSciNet  MATH  Google Scholar 

  24. Nieto JJ: Impulsive resonance periodic problems of first order. Applied Mathematics Letters 2002, 15(4):489–493. 10.1016/S0893-9659(01)00163-X

    Article  MathSciNet  MATH  Google Scholar 

  25. Di Piazza L, Satco B: A new result on impulsive differential equations involving non-absolutely convergent integrals. Journal of Mathematical Analysis and Applications 2009, 352(2):954–963. 10.1016/j.jmaa.2008.11.048

    Article  MathSciNet  MATH  Google Scholar 

  26. Shen J, Wang W: Impulsive boundary value problems with nonlinear boundary conditions. Nonlinear Analysis: Theory, Methods & Applications 2008, 69(11):4055–4062. 10.1016/j.na.2007.10.036

    Article  MathSciNet  MATH  Google Scholar 

  27. Yao M, Zhao A, Yan J: Periodic boundary value problems of second-order impulsive differential equations. Nonlinear Analysis: Theory, Methods & Applications 2009, 70(1):262–273. 10.1016/j.na.2007.11.050

    Article  MathSciNet  MATH  Google Scholar 

  28. Feng M, Du B, Ge W: Impulsive boundary value problems with integral boundary conditions and one-dimensional -Laplacian. Nonlinear Analysis: Theory, Methods & Applications 2009, 70(9):3119–3126. 10.1016/j.na.2008.04.015

    Article  MathSciNet  MATH  Google Scholar 

  29. Kristály A, Rădulescu V, Varga C: Variational Principles in Mathematical Physics, Geometry, and Economics: Qualitative Analysis of Nonlinear Equations and Unilateral Problems, Encyclopedia of Mathematics and its Applications, No. 136. Cambridge University Press, Cambridge, UK; 2010.

    Book  MATH  Google Scholar 

  30. Cabada A, Tomeček J: Extremal solutions for nonlinear functional -Laplacian impulsive equations. Nonlinear Analysis: Theory, Methods & Applications 2007, 67(3):827–841. 10.1016/j.na.2006.06.043

    Article  MathSciNet  MATH  Google Scholar 

  31. Zhang Q, Qiu Z, Liu X: Existence of solutions and nonnegative solutions for weighted -Laplacian impulsive system multi-point boundary value problems. Nonlinear Analysis: Theory, Methods & Applications 2009, 71(9):3814–3825. 10.1016/j.na.2009.02.040

    Article  MathSciNet  MATH  Google Scholar 

  32. Yang Z: Existence of nontrivial solutions for a nonlinear Sturm-Liouville problem with integral boundary conditions. Nonlinear Analysis: Theory, Methods & Applications 2008, 68(1):216–225. 10.1016/j.na.2006.10.044

    Article  MathSciNet  MATH  Google Scholar 

  33. Li Y, Li F: Sign-changing solutions to second-order integral boundary value problems. Nonlinear Analysis: Theory, Methods & Applications 2008, 69(4):1179–1187. 10.1016/j.na.2007.06.024

    Article  MathSciNet  MATH  Google Scholar 

  34. Ma R, An Y: Global structure of positive solutions for nonlocal boundary value problems involving integral conditions. Nonlinear Analysis: Theory, Methods & Applications 2009, 71(10):4364–4376. 10.1016/j.na.2009.02.113

    Article  MathSciNet  MATH  Google Scholar 

  35. Zhang X, Yang X, Ge W: Positive solutions of th-order impulsive boundary value problems with integral boundary conditions in Banach spaces. Nonlinear Analysis: Theory, Methods & Applications 2009, 71(12):5930–5945. 10.1016/j.na.2009.05.016

    Article  MathSciNet  MATH  Google Scholar 

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Acknowledgments

This paper is partly supported by the National Science Foundation of China (10701066, 10926075, and 10971087), China Postdoctoral Science Foundation funded project (20090460969), and the Natural Science Foundation of Henan Education Committee (2008-755-65).

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Dong, R., Guo, Y., Zhao, Y. et al. Existence of Solutions for a Weighted -Laplacian Impulsive Integrodifferential System with Multipoint and Integral Boundary Value Conditions. J Inequal Appl 2010, 392545 (2010). https://doi.org/10.1155/2010/392545

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