Abstract
Based on fixed point index, the paper develops a theory of existence, localization and multiplicity of solutions to first-order differential systems subject to linear nonlocal conditions.
The main features concern the role of the support of the nonlocal condition and the positivity of solutions which is only required on a prescribed subinterval.
Several examples of problems admitting at least one, two, or sequences of such solutions are included, and numerical solutions are obtained using the Mathematica shooting program with starting initial conditions suggested by the theoretical localization results.
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V. Ilea, A. Novac, D. Otrocol, R. Precup, Solutions with a prescribed interval of positivity for differential systems with nonlocal conditions, Appl. Math. Comput., 375 (2020), doi: 10.1016/j.amc.2020.125092
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[1] D.R. Anderson, Existence of three solutions for a first-order problem with nonlinear nonlocal boundary conditions, J. Math. Anal. Appl. 408 (2013) 318–323.
[2] A. Boucherif, R. Precup, On nonlocal initial value problems for first order differential equations, Fixed Point Theory 4 (2003) 205–212.
[3] O. Bolojan-Nica, G. Infante, R. Precup, Existence results for systems with coupled nonlocal initial conditions, Nonlinear Anal. 94 (2014) 231–242.
[4] T. Cardinali, R. Precup, P. Rubbioni, A unified existence theory for evolution equations and systems under nonlocal conditions, J. Math. Anal. Appl. 432 (2015) 1039–1057.
[5] N. Cioranescu, Sur les conditions linéaires dans l’intégration des équations différentielles ordinaires, Math. Z. 35 (1932) 601–608.
[6] R. Conti, Recent trends in the theory of boundary value problems for ordinary differential equations, Boll. Un. Mat. Ital. 22 (1967) 135–178.
[7] K. Deimling, Nonlinear Functional Analysis, Springer, Berlin, 1985.
[8] D.-R. Herlea, Existence and localization of positive solutions to first order differential systems with nonlocal conditions, Stud. Univ. Babes¸ -Bolyai Math. 59 (2014) 221–231.
[9] J. Mawhin, K. Szymanska-Debowska, Convex sets, fixed points and first order systems with nonlocal boundary conditions at resonance, J. Nonlinear Convex Anal. 18 (2017) 149–160.
[10] O. Nica, R. Precup, On the non-local initial value problems for first order differential systems, Stud. Univ. Babes¸ -Bolyai Math. 56 (2011) 113–125.
[11] A. Novac, R. Precup, Theory and computation for multiple positive solutions of non-local problems at resonance, J. Appl. Anal. Comput. 8 (2018) 486–497.
[12] S.K. Ntouyas, Nonlocal initial and boundary value problems: a survey, in: A. Cañada, P. Drábek, A. Fonda (Eds.), Handbook of Differential Equations: Ordinary Differential Equations. Vol 2, Elsevier, Amsterdam, 2005, pp. 461–557.
[13] G. Infante, Positive solutions of nonlocal boundary value problems with singularities, Discrete Contin. Dyn. Syst., 7th AIMS Conference, suppl. (2009) 377–384.
[14] R. Precup, D. Trif, Multiple positive solutions of non-local initial value problems for first order differential systems, Nonlinear Anal. 75 (2012) 5961–5970.
[15] A. Štikonas, A survey on stationary problems, Green’s functions and spectrum of Sturm–Liouville problem with nonlocal boundary conditions, Nonlinear Anal. Model. Control 19 (2014) 301–334.
[16] J.R.L. Webb, G. Infante, Positive solutions of nonlocal initial boundary value problems involving integral conditions, NoDEA Nonlinear Differ. Eq. Appl. 15 (2008) 45–67.
[17] W.M. Whyburn, Differential equations with general boundary conditions, Bull. Amer. Math. Soc. 48 (1942) 692–704.
[18] M. Zima, Positive solutions for a nonlocal resonant problem of first order, in: P. Drygas,S. Rogosin (Eds.), Modern Problems in Applied Analysis, Birkhäuser, 2018, pp. 203–2
Solutions with a prescribed interval of positivity for differential systems with nonlocal conditions
Abstract.
Based on fixed point index, the paper develops a theory of existence, localization and multiplicity of solutions to first-order differential systems subject to linear nonlocal conditions. The main features concern the role of the support of the nonlocal condition and the positivity of solutions which is only required on a prescribed subinterval. Several examples of problems admitting at least one, two, or sequences of such solutions are included, and numerical solutions are obtained using the Mathematica shooting program with starting initial conditions suggested by the theoretical localization results.
Key words: differential system, nonlocal condition, positive solution, multiple solutions, fixed point index
Mathematics Subject Classification: 34B18, 47H11, 47H30
1. Introduction
Many mathematical models arising from physics, chemistry, biology, economics etc. are given by first-order differential systems whose time-dependent variables stay for specific quantities, most often subject by their nature to the condition of positivity. In this connection, there is a huge literature on positive solutions to various classes of problems. However, there are cases where the positivity is only required on a subinterval of time. For instance, in case of the Lotka-Volterra predator-prey model, we may be interested that the size of the prey population on a given time interval - for example the reproduction season - be larger than a given threshold and the size of predator population on that time interval be less than Under the substitutions and the desired threshold conditions become the positivity conditions and on the prescribed time interval Analogous problems appear in economic models when the size of production of some goods in some periods of the year needs to be sufficiently larger to satisfy the market demand, or on the contrary, to be sufficiently smaller to avoid excessive stocks. Having in mind these examples as a main motivation, in this paper we seek solutions to differential systems on a given interval, which are necessarily positive only on a prescribed subinterval.
Additionally in this paper, we treat differential systems with nonlocal conditions. In particular, they include the initial value condition, boundary value conditions, multi-point and integral constraints. As a motivating example, we have the integral condition which appears in many physical models where is a probability distribution. The research on differential equations with nonlocal conditions began with the pioneer works of Cioranescu [5], Whyburn [17] and Conti [6], and have gained a special attention in the last decades motivated by concrete applications in different domains (see, e.g., [1]-[4], [8]-[16] and [18]).
More exactly in this paper we study the existence, localization and multiplicity of solutions to the following problem:
(1.1) |
where is a fixed subinterval of is continuous, and a continuous linear mapping. We shall seek solutions
Taking the nonlocal condition can be replaced by
Our approach to problem (1.1) is based on fixed point principles and fixed point index theory, and takes into consideration the support of namely the smallest subinterval such that for every having the same restriction to
Recall that for a closed convex subset of a Banach a subset open in and a completely continuous operator such that on the one can consider the fixed point index of over with respect to which is denoted by (see, e.g., [7, p. 238]) and has the following properties: implies that has at least one fixed point in (existence);for the any constant operator (normalization); the homotopy invariance; and additivity with respect to We have the following lemma that is used in the proof of our main result.
Lemma 1.1.
If is bounded, convex, open in and then
Proof.
Since one has on the so the index is defined. Let be arbitrarily fixed. Then the homotopy is admissible since for all due to the convexity of Finally, by the homotopy invariance and the normalization properties of the index, we have
∎
Basic notations. We conclude the introduction by some nonstandard notations for vectors and vector-valued functions that will be used throughout the paper. First we make the convection that all vectors in are identified to column matrices, and for two vectors we let if ( respectively) for Also by we mean the vector of components , and by the notation we mean that the -th components of the two vectors satisfy the inequality
We shall use the notation for the matrix whose columns are
Thus, in virtue of the linearity of for any constant vector-valued function using the decomposition
one has that is the product of matrix with the column vector i.e.,
(1.2) |
Also the notation will stay for the identity matrix of size
Finally, for a vector by we shall mean the column vector whose elements are for a scalar function we shall denote by its supremum norm, and for a vector-valued function of scalar components we shall denote by the column vector of elements Also, for any subinterval of by we shall mean the column vector of the elements Thus, when referred to vectors or vector-valued functions, the equalities and inequalities from below have to be seen as equalities and inequalities between column vectors.
2. Main result
First, if the matrix is non-singular, then our differential system subject to the condition is equivalent to the integral type equation in namely
(2.1) |
To prove this it suffices to integrate the differential equation from to an arbitrary to obtain
(2.2) |
then to apply the linear mapping and use the condition to obtain
whence
The solutions of (2.1) are the fixed points of the operator given by
which is completely continuous due to the continuity of and
Looking for solutions that are positive on the prescribed subinterval of we are let to consider the set
Obviously, is a wedge (i.e., closed, convex and with for every ). In order to use fixed point principles and index, we need that the condition is satisfied. It is easily seen that this happens if additionally the following positivity properties hold:
(2.3) |
(2.4) |
(2.5) |
where is the support of Thus is not necessarily positive on for but is positive even for functions which are not positive on the whole interval Also note that under condition (2.4), one has and then the hypothesis (2.5) is equivalent to the fact that the eigenvalues of the matrix are located inside the unit circle.
Our main result is the following theorem on the existence, localization and multiplicity of solutions to problem (1.1).
For two vectors with and we denote:
Also and are the vector-valued functions of the corresponding scalar functions from the above table. For instance,
which is looked as a column vector.
Theorem 2.1.
- :
- :
- :
Proof.
Consider the bounded closed convex subset of
We use the fixed point index of the operator over a number of open sets in and with respect to
() First we prove that under condition (: ), one has which, according to Lemma 1.1 guarantees that the fixed point index of over with respect to is equal to one, i.e., Hence has at least one fixed point in that is a solution as wished. Notice that the existence of a fixed point also follows from Schauder’s fixed point theorem. For doing estimations on it is convenient to represent as sum of two operators, where
and to recall the notations introduced before the statement of the theorem.
First we estimate from above For and we have that for every and so
Then, using (2.4) and the linearity of we deduce that
which together with (2.5) yields
(2.10) |
Next we estimate from above for For we still have for every and so
(2.11) |
For since is not necessarily positive, we only have Hence
(2.12) |
Now (2.11), (2.12) and (2) give
(2.14) |
From (2.10) and (2.14) we deduce the final estimate from above
which together with condition (: ) shows that Thus the proof of () is finished.
() Let
The set is open in We prove that which implies whence the conclusion. To this aim we need to estimate from below. Thus, for
and for Hence, from (2.7) we have that as desired.
() Now consider the set
Clearly, the set is open in and the sets and are disjoint. Since we have for , and for Then from (: ) and (: ), we see that
Then, as at case (), we may infer that and so Hence a second fixed point exists in
In the end, from
we find a third fixed point in The localization properties of the three solutions come from the definitions of the sets and ∎
Remark 2.1.
Under the assumptions of Theorem 2.1 (), the solutions and are different from zero. If in addition then the solution is also different from zero.
Remark 2.2.
For only one autonomous equation (), conditions (: ), (2.7) and (: ) read as:
In particular, if
(2.15) |
the above inequalities reduce to
(2.16) |
(2.17) |
(2.18) |
showing the oscillation of the function
Notice the dependence of the numbers and on the support of the mapping through the values and Also note a sufficient condition for (2.15) to hold, namely that is nonnegative and increasing on and is odd or even on for some
Example 2.1.

It is easy to show that the function is positive and increasing on Hence (2.15) holds whatever would be and Such numbers with and satisfying (2.16) and (2.17) exist since
The result then follows from Theorem 2.1 (). We underline the fact that the solution is not positive on the whole interval but, as predicted by our theory, it is positive on the subinterval the support of the nonlocal condition.
Example 2.2.
Consider the problem
(2.19) |
For
the problem has at least one solution with on
Indeed, the function is even on and nonnegative, increasing on since hence (2.15) holds whatever will be and We have and then and Also and Looking for a number with we are led to the inequality which has positive solutions for Finally, a number can be found since as The conclusion follows from Theorem 2.1 ().
Example 2.3.
For
and sufficiently small problem (2.19) has at least three nonzero solutions. As in the previous example, the function is even on and nonnegative, increasing on hence (2.15) holds whatever would be and Also and First we prove that there are two numbers and with such that and that is
(2.20) | |||||
Since there is with which makes true the second inequality in (2.20) for every Next we choose such that and then such that Thus conditions (2.20) are fulfilled. Finally, since as there exists such that From Theorem 2.1 (), the problem has three solutions with
(2.21) |
These solutions are nonzero since To test our theoretical result, we consider and Then the conditions on the three radii and are fulfilled by the values and using the Shooting program of Mathematica, we obtain three numerical solutions satisfying (2.21), as shown in Figure 2.

Example 2.4.
For
and any problem (2.19) has a sequence of solutions with If then in addition there exists a sequence of nonzero solutions with
The function is nonnegative and increasing on and is odd on Hence (2.15) holds. As in the previous two examples, one have and Since
there exist sequences and tending to and such that
Hence, from Theorem 2.1 (), for each the problem has a solution with From
and we find that For two such solutions are numerically obtained with the Shooting program of Mathematica, and are represented in Figure 3.

If then we also have
Consequently, there exist sequences and tending to and such that
for all Then for each there is a solution satisfying and Clearly from and we have that
Example 2.5.
Consider the following problem related to a bidimensional system
(2.22) |
If
and the problem has at least one solution satisfying on . In this case we have
and Also, taking and the vector conditions in Theorem 2.1 () are
Explicitly, the first condition gives
(2.23) |
where Since for both one has as such a number exists sufficiently large. The second vector condition gives
(2.24) |
where These inequalities yield to the system
which has a positive solution if and Thus Theorem 2.1 () applies and gives the conclusion.
Example 2.6.
Consider problem (2.22) where
For each number and any large enough the problem has at least three nonzero solutions. Indeed, with the notations from the previous example, the conditions (2.24) are satisfied for sufficiently large and Next conditions (2.23) allow us to find large enough since for both one has as Now we put so and we look for such that the additional condition in Theorem 2.1 () is satisfied. Thus, we need that
Such a number exists since as Now the conclusion follows from Theorem 2.1 ().
In the above examples we have considered autonomous equations. We emphasize the more general applicability of Theorem 2.1 to nonautonomous equations, as the following example shows.
Example 2.7.
In problem (2.19), consider the -depending function
As in Example 2.3, if and is sufficiently small, there exists at least three nonzero solutions. Indeed, by direct computation involving maximization and minimization of also with respect to one can see that conditions (: ) and (2.7) of Theorem 2.1 are satisfied providing that
(2.25) | |||||
Similarly to Example 2.3, these inequalities make possible the choice of and In addition, condition (: ) is fulfilled by a sufficiently large
References
- [1] D.R. Anderson, Existence of three solutions for a first-order problem with nonlinear nonlocal boundaryconditions, J. Math. Anal. Appl., 2013, 408, 318–323.
- [2] A. Boucherif and R. Precup, On nonlocal initial value problems for first order differential equations, Fixed Point Theory, 2003, 4, 205–212.
- [3] O. Bolojan-Nica, G. Infante and R. Precup, Existence results for systems with coupled nonlocal initial conditions, Nonlinear Anal., 2014, 94, 231–242.
- [4] T. Cardinali, R. Precup and P. Rubbioni, A unified existence theory for evolution equations and systems under nonlocal conditions, J. Math. Anal. Appl., 2015, 432, 1039–1057.
- [5] N. Cioranescu, Sur les conditions linéaires dans l’intégration des équations différentielles ordinaires, Math. Z., 1932, 35, 601–608.
- [6] R. Conti, Recent trends in the theory of boundary value problems for ordinary differential equations, Boll. Un. Mat. Ital., 1967, 22, 135–178.
- [7] K. Deimling, Nonlinear Functional Analysis, Springer, Berlin, 1985.
- [8] D.-R. Herlea, Existence and localization of positive solutions to first order differential systems with nonlocal conditions, Stud. Univ. Babeş-Bolyai Math., 2014, 59, 221–231.
- [9] J. Mawhin and K. Szymanska-Debowska, Convex sets, fixed points and first order systems with nonlocal boundary conditions at resonance, J. Nonlinear Convex Anal., 2017, 18, 149–160.
- [10] O. Nica and R. Precup, On the non-local initial value problems for first order differential systems, Stud. Univ. Babeş-Bolyai Math., 2011, 56, 113–125.
- [11] A. Novac and R. Precup, Theory and computation for multiple positive solutions of non-local problems at resonance, J. Appl. Anal. Comput., 2018, 8, 486–497.
- [12] S.K. Ntouyas, Nonlocal initial and boundary value problems: a survey, in: Handbook of Differential Equations: Ordinary Difeential Equations. Vol 2, A. Cañada, P. Drábek and A. Fonda (Eds.), Elsevier, Amsterdam, 2005, pp. 461–557.
- [13] G. Infante, Positive solutions of nonlocal boundary value problems with singularities, Discrete Contin. Dyn. Syst., 2009, Supplement, 377–384.
- [14] R. Precup and D. Trif, Multiple positive solutions of non-local initial value problems for first order differential systems, Nonlinear Anal., 2012, 75, 5961–5970.
- [15] A. Štikonas, A survey on stationary problems, Green’s functions and spectrum of Sturm–Liouville problem with nonlocal boundary conditions, Nonlinear Anal. Model. Control, 2014, 19, 301–334.
- [16] J.R.L. Webb and G. Infante, Positive solutions of nonlocal initial boundary value problems involving integral conditions, NoDEA Nonlinear Differential Equations Appl., 2008, 15, 45–67.
- [17] W.M. Whyburn, Differential equations with general boundary conditions, Bull. Amer. Math. Soc., 1942, 48, 692–704.
- [18] M. Zima, Positive solutions for a nonlocal resonant problem of first order, in Modern Problems in Applied Analysis, P. Drygaś, S. Rogosin (Eds.), Birkhäuser, 2018, pp. 203–214.