A Note on a Beam Equation with Nonlinear Boundary Conditions
 Paolamaria Pietramala^{1}Email author
DOI: 10.1155/2011/376782
© Paolamaria Pietramala. 2011
Received: 14 May 2010
Accepted: 31 July 2010
Published: 12 August 2010
Abstract
We present new results on the existence of multiple positive solutions of a fourthorder differential equation subject to nonlocal and nonlinear boundary conditions that models a particular stationary state of an elastic beam with nonlinear controllers. Our results are based on classical fixed point index theory. We improve and complement previous results in the literature. This is illustrated in some examples.
1. Introduction
that models a bar with the left end being simply supported (hinged) and the right end being sliding clamped. This problem, and its generalizations, has been studied previously by Davies and coauthors [2], Graef and Henderson [3] and Yao [4].
model a bar where the displacement and the bending moment at are zero, and there are relations, not necessarily linear, between the shearing force and the angular attitude at and the displacement in two other points of the beam.
involving RiemannStieltjes integrals.
The conditions (1.5)(1.6) cover a variety of cases and include, as special cases when , multipoint and integral boundary conditions. These are widely studied objects in the case of fourthorder BVPs; see, for example, [5–14]. BCs of nonlinear type also have been studied before in the case of fourthorder equations; see, for example, [15–20] and references therein.
The study of positive solutions of BVPs that involve Stieltjes integrals has been done, in the case of positive measures, in [21–24]. Signed measures were used in [12, 25]; here, as in [21, 22], due to some inequalities involved in our theory, the functionals are assumed to be given by positive measures.
with suitable functions .
and gives a simple general method to avoid long technical calculations.
In our paper the approach of [21] is applied to BVP (1.1)–(1.6): we rewrite this BVP as a perturbed Hammerstein integral equation, and we prove the existence of multiple positive solutions under a suitable oscillatory behavior of the nonlinearity . We observe that our results are new even for the local BCs, when . We illustrate our theory with some examples. We also point out that this approach may be utilized for other sets of nonlinear BCs that have a physical interpretation, this is done in the last section.
2. The Boundary Value Problem
here we look for a better , since this enables us to weaken the growth requirements on the nonlinearity .
An upper bound for is obtained by finding for each fixed . Since for , is a nondecreasing function of that attains its maximum, for each fixed , when .
and we show that we can study this problem by means of a perturbation of the Hammerstein integral equation (2.2).
and we work in a suitable cone in the Banach space of continuous functions defined on the interval endowed with the usual supremum norm.
Our assumptions are the following:
, almost everywhere, and ;
for every ;
involving Stieltjes integrals with positive measures ;
, and .
and to use the classical fixed point index for compact maps (see e.g., [29] or [30]).
We observe, as in [21], that leaves invariant and is compact. We give the proof in the Carathéodory case for completeness.
Lemma 2.1.
If the hypotheses hold, then maps into . Moreover, is a compact map.
Proof.
Hence we have . Moreover, the map is compact since it is a sum of two compact maps: the compactness of is well known, and since , and are continuous, the perturbation maps bounded sets into bounded subsets of a 1dimensional space.
Note that .
The proofs of the following results can be immediately deduced from the analogous results in [21], where the proofs involve a careful analysis of fixed point index and utilize orderpreserving matrices. The only difference here is that we allow nonlinearity to be Carathéodory instead of continuous. The lines of proof are not effected and therefore the proofs are omitted.
Firstly we give conditions which imply that the fixed point index is on the set .
Lemma 2.2.
Then the fixed point index, , is .
Now, we give conditions which imply that the fixed point index is on the set .
Lemma 2.3.
Then .
The two lemmas above lead to the following result on existence of one or two positive solutions for the integral equation (2.20). Note that, if the nonlinearity has a suitable oscillatory behavior, it is possible to state, with the same arguments as in [23], a theorem on the existence of more than two positive solutions.
Theorem 2.4.
Suppose hold. Let and be as in (2.26). Then (2.20) has one positive solution in if either of the following conditions holds:
there exist with such that (2.34) is satisfied for and (2.33) is satisfied for ;
there exist with such that (2.33) is satisfied for and (2.34) is satisfied for .
Equation (2.20) has at least two positive solutions in if one of the following conditions hold.
there exist , with , such that (2.34) is satisfied for , (2.33) is satisfied for , and (2.34) is satisfied for ;
there exist , with and , such that (2.33) is satisfied for , (2.34) is satisfied for , and (2.33) is satisfied for .
3. Optimal Constants and Examples
with the BCs (1.4)–(1.6).
We seek the "optimal" for which is a minimum. This type of problems has been tackled in the past, for example, in the secondorder case for heatflow problems in [32] and for beam equations (under different BCs) in [9, 12, 13].
Such maximum is attained at . Thus the "optimal" interval , for which is a minimum, is the interval ; this gives and .
Remark 3.1.
For example, with and , the BVP (3.5) has at least two positive solutions in if there exist , such that , and .
These results are new and improve and complement the previous ones. Gupta [1] and Yao [4] studied the problem with more general nonlinearity but established existence results only. Davies and coauthors [2] and Graef and Henderson [3] obtain the existence of multiple positive solutions for a order differential equation subject to our boundary conditions in the case . In [2] the choice gives the values and which replace our constants and in the growth conditions of . The growth conditions of the nonlinearity in Theorem in [3] cannot be compared with ours, but we do not require the restriction .
The next examples illustrate the applicability of our results. Firstly we consider, as an illustrative example, the case of a nonlinear point problem.
Example 3.2.
and conditions (2.34) and (2.33) read and . Since holds, from Theorem 2.4 it follows that this BVP has a nontrivial solution in . A nonlinearity that easily verifies , for example, is the function for every and every .
We now give an example with continuously distributed positive measures.
Example 3.3.
and conditions (2.34) and (2.33) read and .
4. Other Nonlinear BCs
As in [12], where a different set of BCs were investigated, we point out that these nonlocal boundary conditions can be interpreted as feedback controls: for example, the BCs (4.1) can be seen as a control on the displacement at the left end and a device handling the shear force at .
Table 1
BCs (1.4)–(1.6)  BCs (4.1)  BCs (4.2)  BCs (4.3)  BCs (4.4)  BCs (4.5)  





























the cone , given by the constant , varies according to the nonhomogeneous BCs considered. This affects also, in a natural manner, conditions (2.33) and (2.34).
Declarations
Acknowledgments
The author would like to thank professor Salvatore Lopez of the Faculty of Engineering, University of Calabria, for shedding some light on the physical interpretation of this problem. The author wishes to thank the anonymous referees for their constructive comments.
Authors’ Affiliations
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