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First order differential systems with a nonlinear boundary condition via the method of solution-regions
Boundary Value Problems volume 2021, Article number: 19 (2021)
Abstract
In this article we extend the known theory of solution regions to encompass nonlinear boundary conditions. We both provide results for new boundary conditions and recover some known results for the linear case.
1 Introduction
In this paper, we study systems of differential equations with nonlinear boundary conditions of the form:
where \(f: [0,T] \times \mathbb{R}^{n} \to \mathbb{R}^{n}\) is a Carathéodory function and \(L: \mathbb{R}^{2n}\times C(I,\mathbb{R}^{n}) \to \mathbb{R}^{n}\) is continuous.
To our knowledge, few results can be found in the literature in the case where \(n > 1\) and L is nonlinear or does not depend only on the values at the boundary, \(u(0)\) and \(u(T)\). In [17] and [18], this problem was treated with linear integral boundary conditions. Results were obtained in the case where f satisfies a growth condition or a condition of contraction type.
The problem (1.1) in the case of a single differential equation (\(n=1\)) and L nonlinear of the form \(L(x,y,u) = L(x,y)\) was studied by [1, 2, 4, 15]. Existence results were obtained with the method of upper and lower solutions and under monotonicity conditions imposed on L.
In a recent work of Frigon [7], the concept of solution-region was introduced for the first time in order to obtain results concerning the existence and multiplicity of solutions of the system of differential equations (1.1) in the particular case of the initial condition
or the periodic boundary condition
This method of solution-region was extended by Tojo in [20] to treat more general linear boundary conditions such as
where \(r\in {\mathbb{R}^{n}}\) and \(\Gamma: C([0,T],{\mathbb{R}^{n}})\to {\mathbb{R}^{n}}\) is a linear functional such that
(with 1 understood as the constant function 1 on \([0,T]\)).
This new method generalizes various means of obtaining existence and multiplicity of solutions of differential problems, such as the methods of upper and lower solutions [1, 2, 4, 9, 15, 16], strict upper and lower solutions [13, 19], and solution-tubes [3, 6, 8, 10]. Furthermore, the method is closely related to that of Gaines and Mawhin concerning what they called bound sets [11, 12]. The theory of bound sets was developed for the case where f is a continuous map and their existence results are obtained for bound sets not depending on t.
In this paper, we improve the works [7, 20] by studying systems of differential equations with nonlinear boundary conditions such as (1.1). The results obtained recover, in most cases, the results in [7, 20] for the case of linear boundary conditions. We also sharpen the definition and requirements for a set to be considered a solution-region (see Definition 3.1) for the case of nonlinear boundary conditions when compared to the linear one present in the literature (cf. [7, 20]). It is worthwhile to mention that no monotonicity or growth conditions will be imposed on f and L.
The paper is structured as follows. In Sect. 2 we deal with some preliminaries that we will use afterwards. Section 3 is concerned with the main results of this work and contains detailed applications that render already known results, thus showing the generality of our approach. Finally, in Sect. 4, we draw some conclusions regarding future work.
2 Preliminaries
Throughout this paper, we consider \({\mathbb{R}}^{n}\) with the Euclidean norm \(\|\cdot \|\), \({C}(\Omega, \mathbb{R}^{n})\), the space of continuous functions endowed with supremum norm \(\|\cdot \|_{\infty }\), and \(L^{1}(I,\mathbb{R})\) is the space of Lebesgue integrable functions endowed with the usual norm \(\|\cdot \|_{1}\), where \(I=[0,T]\) and Ω is some set. We consider also the Sobolev space \(W^{1,1}(I,\mathbb{R}^{n})\) and, for \(J \subset I\), the following set of locally absolutely continuous maps:
We recall the notion of locally Carathéodory functions introduced in [7].
Definition 2.1
Let \(D \subset I \times {\mathbb{R}}^{n}\). A map \(f: D \to \mathbb{R}^{m}\) is a Carathéodory function if
-
(i)
\(f(t,\cdot )\) is continuous on \(\{x: (t,x) \in D\}\) for almost every \(t \in I\);
-
(ii)
\(f(\cdot,x)\) is measurable for all \(x \in \{t: (t,x) \in D\}\);
-
(iii)
for all \(k > 0\), there exists \(\psi _{k} \in L^{1}(I,\mathbb{R})\) such that \(\|f(t,x)\| \leqslant \psi _{k}(t)\) for a.e. t and every x such that \(\|x\| \leqslant k\) and \((t,x) \in D\).
A map \(f: D \to \mathbb{R}^{m}\) is locally Carathéodory if \(f|_{A}\) is a Carathéodory function for every compact set \(A \subset D\).
It is well known that a completely continuous operator is associated to a Carathéodory map.
Lemma 2.2
([5])
Let \(g: I \times {\mathbb{R}}^{n} \to {\mathbb{R}}^{n}\) be a Carathéodory function and \(N_{g}:{C}(I,{\mathbb{R}}^{n}) \to {C}(I,{\mathbb{R}}^{n})\) the operator defined by
Then, \(N_{g}\) is continuous and completely continuous.
The following comparison result will be useful to ensure that solutions are in a given set.
Lemma 2.3
([7])
Let \(w: [a,b] \to \mathbb{R}\) be a continuous map and \(J = \{t \in [a,b]: w(t)>0\}\). Assume that
-
(i)
\(w \in W^{1,1}_{\operatorname{loc}}(J,\mathbb{R})\);
-
(ii)
\(w'(t) \leqslant 0\) a.e. \(t \in J\); and
-
(iii)
one of the following conditions holds:
-
(iii.1)
\(w(a) \leqslant 0\);
-
(iii.2)
\(w(a) \leqslant w(b)\).
-
(iii.1)
Then, \(w(t) \leqslant 0\) for all \(t \in [a,b]\) or there exists \(k>0\) such that \(w(t)=k\) for all \(t \in [a,b]\).
In order to present the problem of study, we recall the notion of an admissible region introduced in [7].
Definition 2.4
([7])
We say that a set \(R \subset I \times {\mathbb{R}}^{n}\) is an admissible region if there exist two continuous maps \(h: I \times {\mathbb{R}}^{n} \to \mathbb{R}\) and \(p = (p_{1},p_{2}): I \times {\mathbb{R}}^{n} \to I \times {\mathbb{R}}^{n}\) satisfying the following conditions:
-
(H1)
\(R = \{(t,x): h(t,x) \leqslant 0\}\) is bounded and, for every \(t \in I\), \(R_{t}=\{x\in {\mathbb{R}}^{n}: (t,x)\in R\}\ne \emptyset \);
-
(H2)
the map h has partial derivatives at \((t,x)\) for almost every t and every x with \((t,x) \in R^{c}: = (I\times {\mathbb{R}}^{n} )\backslash R\), and \(\frac{\partial h}{\partial t}\), \(\nabla _{x}h\) are locally Carathéodory maps on \(R^{c}\);
-
(H3)
p is bounded and such that \(p(t,x) =(t,x)\) for every \((t,x) \in R\) and
$$ \bigl\langle \nabla _{x} h(t,x),p_{2}(t,x)-x \bigr\rangle < 0\quad \text{for a.e. $t$ and every $x$ with $(t,x) \in R^{c}$}. $$
We call \((h,p)\) an admissible pair associated to R.
In [20], a weaker notion of admissible region was considered where, in condition (H3), the inequality is taken to be non-strict.
Definition 2.5
We say that a set \(R \subset I \times {\mathbb{R}}^{n}\) is a weak admissible region if there exist two continuous maps \(h: I \times {\mathbb{R}}^{n} \to \mathbb{R}\) and \(p = (p_{1},p_{2}): I \times {\mathbb{R}}^{n} \to I \times {\mathbb{R}}^{n}\) satisfying (H1) and (H2) of Definition 2.4 and
-
(H3)’
p is bounded and such that \(p(t,x) =(t,x)\) for every \((t,x) \in R\) and
$$ \bigl\langle \nabla _{x} h(t,x),p_{2}(t,x)-x \bigr\rangle \leqslant 0, \quad\text{for a.e. $t$ and every $x$ with $(t,x) \in R^{c}$}. $$
We call \((h,p)\) a weak admissible pair associated to R.
3 Solution-regions and nonlinear boundary conditions
We consider systems of first order differential equations of the form:
subject to boundary conditions of the form \(u \in {\mathcal{B}}\) where \({\mathcal{B}} \) denotes one of the following boundary conditions:
where \(f: [0,T]\times {\mathbb{R}}^{n}\to {\mathbb{R}}^{n}\) is a Carathéodory function and \(L: \mathbb{R}^{2n}\times C([0,T],{\mathbb{R}}^{n}) \to {\mathbb{R}}^{n}\) is continuous but not necessarily linear. The boundary conditions (3.2) and (3.3) generalize those considered in [7].
We will be interested in giving conditions ensuring the existence of a solution of (3.1) in a suitable weak admissible region. To this end, we introduce the notion of solution-regions of (3.1).
Definition 3.1
A set \(R \subset I \times {\mathbb{R}}^{n}\) is called a solution-region of (3.1) if it is a weak admissible region with an associated weak admissible pair \((h,p)\) satisfying the following conditions:
-
(i)
for almost every t and every x with \((t,x) \notin R\), one has
$$ \frac{\partial h}{\partial t}(t,x) + \bigl\langle \nabla _{x} h(t,x),f\bigl(p(t,x)\bigr) \bigr\rangle \leqslant 0; $$(3.4)and one of the following conditions:
-
(ii)
If \({\mathcal{B}}\) denotes (3.2), for all \(u \in W^{1,1}(I,{\mathbb{R}}^{n})\) such that \(u(0)= p_{2} (0,u(0)-L(u(0),u(T),u) )\),
-
(a)
\(h(0,u(0))\leqslant 0\);
-
(b)
\((0,u(0)-L(u(0),u(T),u) ) \in R\) if \((t,u(t)) \in R\) for every \(t \in I\).
-
(a)
-
(ii)’
If \({\mathcal{B}}\) denotes (3.3),
-
(a)
\(h(0,u(0)) \leqslant h(T,u(T))\) for every \(u \in W^{1,1}(I,\mathbb{R}^{n})\) such that \((0,u(0)) \notin R\) and \(u(T) - u(0) = tL((u(0),u(T),u))\) for some \(t \in [0,1]\).
-
(b)
The inequality in (ii)’(a) is strict or there exists a set \(S \subset I\) of positive measure such that one of the inequalities in (H3)’ or (3.4) is strict on S.
-
(a)
Now we show that the existence of a solution-region ensures the existence of a solution of (3.1).
Theorem 3.2
Let \(f: I \times {\mathbb{R}}^{n} \to {\mathbb{R}}^{n}\) be a Carathéodory function. Assume that there exists a solution-region R of (3.1). Then, problem (3.1), (3.2) has a solution \(u \in W^{1,1}(I,{\mathbb{R}}^{n})\) such that \((t,u(t)) \in R\) for every \(t \in I\).
Proof
Let \((h,p)\) be a weak admissible pair associated to the solution-region R. For \(\lambda \in [0,1]\), we consider the following family of problems:
![figure a](http://media.springernature.com/lw685/springer-static/image/art%3A10.1186%2Fs13661-021-01495-9/MediaObjects/13661_2021_1495_Figa_HTML.png)
where \(f_{R}: I \times \mathbb{R}^{n} \to \mathbb{R}^{n}\) is defined by
with \(c \in L^{1}(I,\mathbb{R})\) chosen such that
Observe that such a function c exists since f is Carathéodory and p is a bounded map.
Let us consider the operators \(\mathcal{I}_{0}: C(I,\mathbb{R}^{n}) \to \mathbb{R}^{n}\) and \(\mathcal{I}: [0,1]\times C(I,\mathbb{R}^{n}) \to C(I,\mathbb{R}^{n})\) defined by
and
where \(N_{f_{R}}\) is defined in (2.1). Since L is continuous and f is Carathéodory, using (H3)’ of Definition 2.5, we deduce from Lemma 2.2 that \(\mathcal{I}\) is continuous and completely continuous.
We claim that the fixed points of \(\mathcal{I}\) are solutions of (3.5λ). Indeed, if \(u = \mathcal{I}(\lambda,u)\),
In particular, one has, for \(t=0\),
and
Thus, u is a solution of (3.5λ).
Fix \(M > 0\) such that
We show that
Indeed, choose m such that
Assume that u is a solution of (3.5λ) for some \(\lambda \in [0,1]\). If \(\lambda =0\), \(\|u(t)\|= \|\mathcal{I}_{0}(u)\| \leqslant \|p_{2}\|_{\infty }< m\). If \(\lambda \in (0,1]\), then \(\|u(0)\|= \|\mathcal{I}_{0}(u)\| \leqslant \|p_{2}\|_{\infty }< m\) and, from (3.6), (3.7), and (3.10), we deduce that, almost everywhere on \(\{t \in I: \|u(t)\| > m\}\),
Lemma 2.3 implies that \(\|u(t)\| \leqslant m\) for every \(t \in I\) since \(\|u(0)\| \leqslant m\).
Let \(\mathcal{U} = \{u \in C(I,\mathbb{R}^{n}): \|u\|_{\infty }< M\}\). It follows from (3.9) and the homotopy property of the fixed point index that
Observe that
and
By the contraction property of the fixed point index (see [14, Chap. 4, Sect. 12, Theorem 6.2]), one has
Let us define \(H_{0}: [0,1] \times \overline{B_{\mathbb{R}^{n}}(0,M)} \to \mathbb{R}^{n}\) by
It is clear that \(x \ne H_{0}(\lambda,x)\) for every \((\lambda,x) \in [0,1]\times \partial B_{\mathbb{R}^{n}}(0,M)\). The homotopy property of the fixed point index implies that
Combining (3.12), (3.13), and (3.14), one obtains
Therefore, for every \(\lambda \in [0,1]\), \(\mathcal{I}(\lambda,\cdot )\) has a fixed point, and hence (3.5λ) has a solution.
Now let u be a solution of (3.5λ) for \(\lambda =1\). It follows from (3.6) and Definitions 2.5 and 3.1 that, almost everywhere on \(\{t: h(t,u(t)) > 0\}\),
By Definition 3.1(ii)(a), \(h(0,u(0))\leqslant 0\). Lemma 2.3 implies that \(h(t,u(t))\leqslant 0\) for every \(t\in I\), and hence, \((t,u(t)) \in R\) for every \(t \in I\).
So, \(u'(t)=f_{R}(t,x)=f(t,x)\) and equation (3.1) holds. Furthermore, by Definition 3.1(ii)(b), \((0,u(0)-L(u(0),u(T),u) )\in R\). Hence,
Therefore, \(L(u(0),u(T),u)=0\) and condition (3.2) holds. We conclude that u is a solution of (3.1), (3.2). □
We present an example of application of the previous theorem in which there are no monotonicity assumptions or growth conditions imposed on the right-hand side term of (3.1) or in (3.2).
Example 3.3
We consider the following system of differential equations:
Let \(L: \mathbb{R}^{4}\times C([0,1],\mathbb{R}^{2}) \to \mathbb{R}^{2}\) be defined by
We consider the closed and bounded set
We define \(h: [0,1] \times \mathbb{R}^{2} \to \mathbb{R}\) and \(p: [0,1]\times \mathbb{R}^{2} \to [0,1]\times \mathbb{R}^{2}\) by
and
It is easy to verify that R is an admissible region with the associated admissible pair \((h,p)\).
To show that R is a solution-region of (3.15), we need to verify (3.4) (see Fig. 1). For \((t,x) \notin R\), one has
Observe that
and
So,
Observe that \(h(0,p_{2}(0,x)) = h(p(0,x)) \leqslant 0\) for every \(x \in \mathbb{R}^{2}\). In particular, if \(u \in W^{1,1}([0,1],\mathbb{R}^{2})\) is such that \(u(0) = p_{2} (0,u(0)-L(u(0),u(1),u) )\), then \(h(0,u(0)) \leqslant 0\). In addition, if \((t,u(t)) \in R\) for every \(t \in [0,1]\), then \(|u_{1}(t)| \leqslant 3/(3-t)\), \(|u_{2}(t)| \leqslant 2/(2-t)\),
and
Hence, \((0,u(0)-L(u(0),u(1),u) ) \in R\). We have shown that condition (ii) of Definition 3.1 is satisfied. It follows from Theorem 3.2 that (3.15) has a solution \(u \in W^{1,1}([0,1],\mathbb{R}^{2})\) such that \((t,u(t)) \in R\) for every \(t \in [0,1]\).
As a corollary of the previous theorem, we obtain an existence result established in [7] for the initial value problem.
Corollary 3.4
Let \(R \subset I\times {\mathbb{R}}^{n}\) be a weak admissible region, \(r \in {\mathbb{R}}^{n}\) and \(f: I \times {\mathbb{R}}^{n} \to {\mathbb{R}}^{n}\) be a Carathéodory function. Assume that there exists \((h,p)\) a weak admissible pair of R satisfying (i) of Definition 3.1and \(h(0,r) \leqslant 0\). Then, (3.1) has a solution \(u \in W^{1,1}(I,{\mathbb{R}^{n}})\) such that \((t,u(t)) \in R\) for every \(t \in I\), and \(u(0)=r\).
Proof
Observe that the initial value problem
is the problem (3.1), (3.2) with \(L(x,y,u)=x-r\). The conclusion will follow from Theorem 3.2 if R is a solution region of (3.1), (3.2). We only need to verify condition (ii) of Definition 3.1. Observe that
By assumption, \(h(0,r) \leqslant 0\). So, \((0,r) \in R\) and Definition 3.1(ii)(b) is satisfied. Moreover, \(p(0,r)=(0,r)\). Therefore, the condition \(u(0)= p_{2} (0,u(0)-L(u(0),u(T),u) )\) in Definition 3.1(ii)(a) turns into \(u(0)=r\). Hence, \(h(0,u(0))\leqslant 0\) and the result holds. □
Theorem 3.2 has also, as a corollary, an existence result for a first order differential equation with a nonlinear boundary condition and under a condition of existence of lower and upper solutions.
Corollary 3.5
Let \(f: I \times \mathbb{R} \to \mathbb{R}\) be a Carathéodory function, \(L: \mathbb{R}^{2}\times {C}(I,\mathbb{R}) \to \mathbb{R}\) be continuous and \(\alpha, \beta \in W^{1,1}(I,\mathbb{R})\) such that
-
(i)
\(\alpha (t) \leqslant \beta (t)\) for every \(t \in I\);
-
(ii)
\(f(t,\beta (t)) \leqslant \beta '(t)\) for almost every \(t \in I\); and \(L(\beta (0),\beta (T),\beta ) \geqslant 0\);
-
(iii)
\(f(t,\alpha (t)) \geqslant \alpha '(t)\) for almost every \(t \in I\); and \(L(\alpha (0),\alpha (T),\alpha ) \leqslant 0\);
-
(iv)
\(L(\alpha (0),u(t),u) \leqslant L(\alpha (0),\alpha (T),\alpha )\) for every \(u \in {C}(I,\mathbb{R})\) such that \(u(0)= \alpha (0)\) and \(\alpha (t) \leqslant u(t) \leqslant \beta (t)\) for every \(t \in I\);
-
(v)
\(L(\beta (0),u(t),u) \geqslant L(\beta (0),\beta (T),\beta )\) for every \(u \in {C}(I,\mathbb{R})\) such that \(u(0)= \beta (0)\) and \(\alpha (t) \leqslant u(t) \leqslant \beta (t)\) for every \(t \in I\).
Then, (3.1), (3.2) has a solution \(u \in W^{1,1}(I,{\mathbb{R}})\) such that \((t,u(t)) \in R\) for every \(t \in I\), with
Proof
As pointed out in [7] (see Examples 3.2 and 4.2), \((h,p)\) where
and
is an admissible pair of R satisfying Definition 3.1(i). Indeed, \(h^{-1}((-\infty,0])=R\) and, by definition of α and β, (H2) holds as well. Finally, for a.e. t and every x with \((t,x) \in R^{c}\), we study two different cases:
-
If \(x<\alpha (t)\), by (iii),
$$\begin{aligned} & \bigl\langle \nabla _{x} h(t,x),p_{2}(t,x)-x \bigr\rangle =-\bigl( \alpha (t)-x\bigr)< 0 \quad\text{and} \\ &\frac{\partial h}{\partial t}(t,x) + \bigl\langle \nabla _{x} h(t,x),f \bigl(p(t,x)\bigr) \bigr\rangle =\alpha '(t)-f\bigl(t,\alpha (t) \bigr)\leqslant 0; \end{aligned}$$ -
If \(x>\beta (t)\),
$$\begin{aligned} & \bigl\langle \nabla _{x} h(t,x),p_{2}(t,x)-x \bigr\rangle =x- \beta (t)< 0 \quad\text{and} \\ &\frac{\partial h}{\partial t}(t,x) + \bigl\langle \nabla _{x} h(t,x),f \bigl(p(t,x)\bigr) \bigr\rangle =-\beta '(t)+f\bigl(t,\alpha (t) \bigr)\leqslant 0. \end{aligned}$$
Hence, \((h,p)\) is an admissible pair and Definition 3.1(i) holds. Finally, observe that \(p_{2}(0,x) \in [\alpha (0),\beta (0)]\) for every \(x \in \mathbb{R}\). Therefore,
Hence, Definition 3.1(ii)(a) is satisfied.
Let \(u \in W^{1,1}(I,\mathbb{R})\) be such that
Assume that \((0,u(0)-L(u(0),u(T),u) ) \notin R\). Without loss of generality,
Then,
and, by (iii) and (iv),
which is a contradiction. Similarly, we get a contradiction if we assume that \(u(0) -L(u(0),u(T),u) > \beta (0)\). So, condition (ii)(b) of Definition 3.1 is satisfied.
Therefore, R is a solution-region of (3.1), (3.2) and the conclusion follows from Theorem 3.2. □
The next corollary is similar (although not comparable) to [20, Theorem 4.9].
Corollary 3.6
Let \(R \subset I\times {\mathbb{R}}^{n}\) be a weak admissible region, \(\Gamma:{C}([a,b],{\mathbb{R}})\to {\mathbb{R}^{n}}\) continuous and \(f: I \times {\mathbb{R}}^{n} \to {\mathbb{R}}^{n}\) be a Carathéodory function. Assume that there exists a weak admissible pair \((h,p)\) of R satisfying (i) of Definition 3.1and
-
(ii)
\(h(0,p_{2}(0,x)) \leqslant 0\) for all \(x \in {\mathbb{R}}^{n}\);
-
(iii)
\((0,u(0) + \Gamma (u) ) \in R\) for every \(u \in W^{1,1}(I,\mathbb{R}^{n})\) such that \((t,u(t)) \in R\) for every \(t \in I\), and \(u(0)=p_{2} (0,u(0) + \Gamma (u) )\).
Then, (3.1) has a solution \(u \in W^{1,1}(I,{\mathbb{R}^{n}})\) such that \((t,u(t)) \in R\) for every \(t \in I\) and \(\Gamma (u) = 0\).
Proof
Let us consider the problem (3.1), (3.2) with \(L(x,y,u)=L(x,u)=-\Gamma (u)\).
To show that R is a solution-region of (3.1), (3.2), we only need to verify condition (ii) of Definition 3.1. Let \(u \in W^{1,1}(I,{\mathbb{R}}^{n})\) be such that \(u(0)=p_{2} (0,u(0)-L(u(0),u) )\). Then
Therefore, by (ii),
and, by (iii),
if, in addition, \((t,u(t)) \in R\) for every \(t \in I\). So, Definition 3.1(ii) is satisfied. Thus, R is a solution-region of (3.1), (3.2). Theorem 3.2 ensures the existence of \(u \in W^{1,1}(I,\mathbb{R}^{n})\) a solution of (3.1) such that \((t,u(t)) \in R\) for every \(t \in I\) and \(\Gamma (u)=0\). □
Here is another corollary of Theorem 3.2 in which a solution of (3.1), (3.2) with the periodic boundary condition is obtained.
Corollary 3.7
Let \(f: I \times \mathbb{R}^{n} \to \mathbb{R}^{n}\) be a Carathéodory function and \(R \subset I\times \mathbb{R}^{n}\) a weak admissible region with an associated weak admissible pair \((h,p)\) satisfying (i) of Definition 3.1and
-
(ii)
\(h(0,p_{2}(0,x)) \leqslant 0\) for all \(x \in \mathbb{R}^{n}\);
-
(iii)
\(h(0,x) \leqslant h(T,x)\) for every x such that \((0,x) \notin R\).
Then, (3.1) has a solution \(u \in W^{1,1}(I,{\mathbb{R}^{n}})\) such that \((t,u(t)) \in R\) for every \(t \in I\) and \(u(0)=u(T)\).
Proof
We consider the problem (3.1), (3.2) with \(L(x,y,u)=x-y\). To show that R is a solution-region, one needs to verify condition (ii) of Definition 3.1. Observe that
Let \(u \in W^{1,1}(I,\mathbb{R}^{n})\) be such that \(u(0)= p_{2} (0,u(0)-L(u(0),u(T),u) )= p_{2}(0,u(T))\). By (ii), we have that
In addition, if \((t,u(t)) \in R\) for every \(t \in I\) and if \((0,u(0)-L(u(0),u(T),u) ) =(0,u(T)) \notin R\), then, by (iii),
This contradicts the fact that \((T,u(T)) \in R\). Thus, R is a solution region of (3.1), (3.2) with \(L(x,y,u) = x-y\). The conclusion follows from Theorem 3.2. □
Remark 3.8
If \(p(0,\cdot )\) is a projection onto \(\{(0,x) \in R\}\), then condition (ii) in Corollaries 3.6 and 3.7 is satisfied.
Observe that, for \(L(x,y,u) = x-y\), the last corollary does not recover the results in [7] for the periodic problem because of condition (ii). The next theorem will show that (ii) of Corollary 3.7 is not necessary if R is an admissible region or if the inequality in Definition 3.1(i) is strict (see Definition 3.1(ii)’(b)).
Theorem 3.9
Let \(f: I \times \mathbb{R}^{n} \to \mathbb{R}^{n}\) be a Carathéodory function. Assume that there exists R, a solution-region of (3.1) with the boundary condition (3.3). Then, the problem (3.1), (3.3) has a solution \(u \in W^{1,1}(I,\mathbb{R}^{n})\) such that \((t,u(t)) \in R\) for every \(t \in I\).
Proof
Let \((h,p)\) be a weak admissible pair associated to the solution-region R. For \(\lambda \in [0,1]\), we consider the following family of problems:
![figure c](http://media.springernature.com/lw685/springer-static/image/art%3A10.1186%2Fs13661-021-01495-9/MediaObjects/13661_2021_1495_Figc_HTML.png)
where \(f_{R}: I \times \mathbb{R}^{n} \to \mathbb{R}^{n}\) is defined in (3.6) and \(L_{R}: \mathbb{R}^{2n} \times {C}(I,\mathbb{R}^{n}) \to \mathbb{R}^{n}\) is given by
Observe that, integrating the equation in (3.16λ) between 0 and T, we have that
which, combined with the boundary conditions in (3.16λ), yields
Let us consider the operator \(\mathcal{P}: [0,1]\times {C}(I,\mathbb{R}^{n}) \to {C}(I,\mathbb{R}^{n})\) defined by
where \(N_{f_{R}}\) is defined in (2.1). As in the proof of the previous theorem, we deduce that \(\mathcal{P}\) is continuous and completely continuous.
We claim that the fixed points of \(\mathcal{P}\) are solutions of (3.16λ). Indeed, if \(u = \mathcal{P}(\lambda,u)\), then, for every \(t \in I\),
In particular, for \(t=0\) and for \(t=T\), we have
Thus,
and (3.18) holds. From (3.18) and (3.19), we deduce that, for almost every \(t \in I\),
Thus, u is a solution of (3.16λ).
Let M and m be as in (3.8) and (3.10), respectively. Assume that u is a solution of (3.16λ) for some \(\lambda \in [0,1]\). If \(\lambda =0\) then
that is, \(u'\) is constant and \(u(T)=u(0)\), so u is constant, say \(u \equiv k\), and
If \(\|k\| > m >1+\|p_{2}\|_{\infty }\geqslant m_{0}+1\), by (3.17),
that is,
Taking norms on both sides of this equality and combining it with (3.7) and (3.10), we obtain
which is a contradiction, so \(\|u(t)\|=\|k\|\leqslant m< M\) for every \(t\in I\).
On the other hand, if \(\lambda \in (0,1]\), combining (3.6), (3.7), (3.10), and (3.18) allows us to deduce that, as in (3.11),
By (3.17) and (3.20), we have that either \(\|u(0)\| \leqslant m\) or \(m<\|u(0)\| = \|u(T)\|\). Taking this into account, it follows from Lemma 2.3 that \(\|u(t)\| \leqslant m\) for every \(t \in I\) since \(\|u\|\) cannot be constant and greater than m. Hence,
Let \(\mathcal{U} = \{u \in {C}(I,\mathbb{R}^{n}): \|u\|_{\infty }< M\}\). It follows from (3.21) and the homotopy property of the fixed point index that
Observe that
and
By the contraction property of the fixed point index, one has
Let us define \(P_{0}: [0,1] \times \overline{B_{\mathbb{R}^{n}}(0,M)} \to \mathbb{R}^{n}\) by
We claim that \(x \ne P_{0}(\lambda,x)\) for every \((\lambda,x) \in [0,1]\times \partial B_{\mathbb{R}^{n}}(0,M)\). Indeed, for \(\lambda =0\) this fact is evident and, if \(\lambda \in (0,1]\), assume that there exists \(x \in \mathbb{R}^{n}\) such that \(\|x\|=M\) and \(x=P_{0}(\lambda,x)\). By (3.6), (3.7), (3.8), and (3.17), it satisfies
So, taking norms on both sides,
which is a contradiction.
The homotopy property of the fixed point index implies that
Combining (3.22), (3.23), and (3.24), we obtain
Therefore, for every \(\lambda \in [0,1]\), \(\mathcal{P}(\lambda,\cdot )\) has a fixed point, and hence (3.16λ) has a solution.
Let u be a solution of (3.16λ) for \(\lambda =1\). It follows from (3.6) and Definitions 2.5 and 3.1 that, almost everywhere on \(\{t: h(t,u(t)) > 0\}\), one has
Since \(u(T)-u(0)=L_{R}(u(0),u(T),u)\), we have that
If \(h(0,u(0)) > 0\), we deduce from Definition 3.1(ii)’(a) that \(h(0,u(0)) \leqslant h(T,u(T))\). Moreover, by Definition 3.1(ii)’(b), this last inequality is strict or the inequality (3.25) is strict on a subset of positive measure. This prevents the existence of \(k>0\) such that \(h(t,u(t)) = k\) for every \(t\in I\). Thus, Lemma 2.3 implies that \((t,u(t)) \in R\) for every \(t \in I\). Therefore, u is a solution of (3.1), (3.3) since \(p=\text{Id}\) on R and \(L_{R}(u(0),u(T),u) = L(u(0),u(T),u)\). □
4 Conclusions
In this work, we have extended the known theory of solution regions to encompass nonlinear boundary conditions and, at the same time, we have recovered some known results for the linear case from our generalization. This was achieved by refining the definition of solution-region for the case of a weak admissible region and nonlinear boundary conditions. Nonetheless, some of the requirements in the definition (see Definition 3.1(ii)’(b)) arise from the fact that in the proof of Theorem 3.9 (see last paragraph) the properties of a weak admissible region are not enough to conclude, something which was indeed the case when solutions regions where defined from admissible regions (cf. [7, Theorem 5.1]).
This raises the question as to whether or why consider weak admissible regions altogether. This laxer definition appeared in [20] in order to prove the following result.
Theorem 4.1
([20])
Let \(R \subset I \times {\mathbb{R}}^{n}\) be a compact set such that the projection of R onto I is surjective. Then, R is a weak admissible region.
This way, weak admissible regions are characterized in a simple topological way, which simplifies the application of the theory. In [20], it was already conjectured that, in fact, all weak admissible regions are admissible regions for an adequate admissible pair. Unfortunately, to the best of our knowledge, there is no proof of that fact as of today. Such a proof would simplify the theory since we could profit from a simple characterization and, at the same time, a simpler definition of solution regions, so it is a result to look forward to.
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References
Cabada, A.: The monotone method for first-order problems with linear and nonlinear boundary conditions. Appl. Math. Comput. 63(2–3), 163–186 (1994)
Cabada, A., Ferreiro, J.B.: First order differential equations with piecewise constant arguments and nonlinear boundary value conditions. J. Math. Anal. Appl. 380(1), 124–136 (2011)
El Khattabi, N., Frigon, M., Ayyadi, N.: Multiple solutions of problems with nonlinear first-order differential operators. J. Fixed Point Theory Appl. 17(1), 23–42 (2015)
Franco, D., Nieto, J.J., O’Regan, D.: Existence of solutions for first order ordinary differential equations with nonlinear boundary. Appl. Math. Comput. 153(3), 793–802 (2004)
Frigon, M.: Théorèmes d’existence de solutions d’inclusions différentielles. In: Topological Methods in Differential Equations and Inclusions. NATO Adv. Sci. Inst. Ser. C Math. Phys. Sci., vol. 472, pp. 51–87. Kluwer Academic, Dordrecht (1995)
Frigon, M.: Systems of first order differential inclusions with maximal monotone terms. Nonlinear Anal., Theory Methods Appl. 66(9), 2064–2077 (2007)
Frigon, M.: Existence and multiplicity results for systems of first-order differential equations via the method of solution-regions. Adv. Nonlinear Stud. 18(3), 469–485 (2018)
Frigon, M., Lotfipour, M.: Multiplicity results for systems of first order differential inclusions. J. Nonlinear Convex Anal. 16, 1025–1040 (2015)
Frigon, M., O’Regan, D.: Existence results for some initial and boundary value problems without growth restriction. Proc. Am. Math. Soc. 123(1), 207–216 (1995)
Frigon, M., O’Regan, D.: Nonlinear first-order initial and periodic problems in Banach spaces. Appl. Math. Lett. 10(4), 41–46 (1997)
Gaines, R.E., Mawhin, J.: Ordinary differential equations with nonlinear boundary conditions. J. Differ. Equ. 26(2), 200–222 (1977)
Gaines, R.E., Mawhin, J.L.: Coincidence Degree, and Nonlinear Differential Equations. Lecture Notes in Mathematics, vol. 568. Springer, Berlin (1977)
Graef, J.R., Kong, L.: Existence of multiple periodic solutions for first order functional differential equations. Math. Comput. Model. 54(11–12), 2962–2968 (2011)
Granas, A., Dugundji, J.: Fixed Point Theory. Springer, New York (2003)
Heikkilä, S., Cabada, A.: On first order discontinuous differential equations with nonlinear boundary conditions. Nonlinear Stud. 3(3), 487–503 (1996)
López Pouso, R.: Nonordered discontinuous upper and lower solutions for first-order ordinary differential equations. Nonlinear Anal., Theory Methods Appl. 45(4), 391–406 (2001)
Mardanov, M.J., Sharifov, Y.A., Ismayilova, K.E., Zamanova, S.A.: Existence and uniqueness of solutions for the system of first-order nonlinear differential equations with three-point and integral boundary conditions. Eur. J. Pure Appl. Math. 12(3), 756–770 (2019)
Mardanov, M.J., Sharifov, Y.A., Molaei, H.H.: Existence and uniqueness of solutions for first-order nonlinear differential equations with two-point and integral boundary conditions. Electron. J. Differ. Equ. 2014, 259 (2014)
Mawhin, J.: First order ordinary differential equations with several periodic solutions. Z. Angew. Math. Phys. 38(2), 257–265 (1987)
Tojo, F.A.F.: A constructive approach towards the method of solution-regions. J. Math. Anal. Appl. 472(2), 1803–1819 (2019)
Acknowledgements
Adrián Tojo would like to thank Professor Marlène Frigon and the Département de Mathématiques et de statistique of the Université de Montréal for their wonderful reception during his stay in the aforementioned department, a time when this paper was started.
Funding
This work was partially supported by NSERC Canada. Marcos Tella and F. Adrián F. Tojo were partially supported by Ministerio de Economía y Competitividad, Spain, and FEDER, project MTM2013-43014-P, and by the Agencia Estatal de Investigación (AEI) of Spain under grant MTM2016-75140-P, co-financed by the European Community fund FEDER.
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Frigon, M., Tella, M. & F. Tojo, F.A. First order differential systems with a nonlinear boundary condition via the method of solution-regions. Bound Value Probl 2021, 19 (2021). https://doi.org/10.1186/s13661-021-01495-9
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DOI: https://doi.org/10.1186/s13661-021-01495-9