
In this paper, we consider some boundary value problems composed by coupled systems of second-order differential equations with full nonlinearities and general functional boundary conditions verifying some monotone assumptions. The arguments apply the lower and upper solutions method, and defining an adequate auxiliary, homotopic, and truncated problem, it is possible to apply topological degree theory as the tool to prove the existence of solution. In short, it is proved that for the parameter values such that there are lower and upper solutions, then there is also, at least, a solution and this solution is localized in a strip bounded by lower and upper solutions. As far as we know, it is the first paper where Ambrosetti-Prodi differential equations are considered in couple systems with different parameters.
Citation: F. Minhós, F. Carapau, G. Rodrigues. Coupled systems with Ambrosetti-Prodi-type differential equations[J]. AIMS Mathematics, 2023, 8(8): 19049-19066. doi: 10.3934/math.2023972
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In this paper, we consider some boundary value problems composed by coupled systems of second-order differential equations with full nonlinearities and general functional boundary conditions verifying some monotone assumptions. The arguments apply the lower and upper solutions method, and defining an adequate auxiliary, homotopic, and truncated problem, it is possible to apply topological degree theory as the tool to prove the existence of solution. In short, it is proved that for the parameter values such that there are lower and upper solutions, then there is also, at least, a solution and this solution is localized in a strip bounded by lower and upper solutions. As far as we know, it is the first paper where Ambrosetti-Prodi differential equations are considered in couple systems with different parameters.
This paper focuses on the search for sufficient conditions to require nonlinearities in order to be able to discuss, depending on the parameters, the existence of solutions for coupled systems of nonlinear second-order differential equations, of the type
{u′′(x)+f(x,u(x),v(x),u′(x),v′(x))=μ m(x),v′′(x)+h(x,u(x),v(x),u′(x),v′(x))=λ n(x), | (E) |
for x∈[0,1], with f,h:[0,1]×R4→R, m,n:[0,1]→R+ continuous functions and μ,λ are real parameter, along with boundary conditions
a1u(0)−b1u′(0)=A1,c1u(1)+d1 u′(1)=B1,a2v(0)−b2v′(0)=A2,c2v(1)+d2v′(1)=B2, | (B) |
where ai,bi,ci,di,Ai,Bi∈R, i=1,2, such that a2i+bi>0, c2i+di>0, for i fixed, and bi,di≥0.
Coupled systems of second-order differential equations were studied by many authors, not only from a mathematical point of view, as in, for example, [1,2,3,4], but also to model some real phenomena, as, for instance, Lokta-Volterra models, reaction diffusion processes, prey-predator systems, Sturm-Liouville problems, mathematical biology, chemical systems, as in [5,6,7,8,9]. Moreover, in the last few years, fractional calculus has had an increasing application to several real processes, as in [10,11,12].
Ambrosetti-Prodi-type problems, introduced in [13,14], have been applied to several types of boundary conditions, as it can be seen in, for example: [15,16], to separated two-point and three-point boundary value problems; [17,18], for Neuman's conditions; [19,20,21,22,23,24] to periodic solutions; [25], for parametric problems with (p,q) -Laplace operator; [26], with asymptotic assumptions; [27], for fractional Laplacian; [28], with asymptotic sign-changed nonlinearities, among others.
Motivated by these works, we consider for the first time, as far as we know, a coupled second-order system composed of two Ambrosetti-Prodi-type differential equations together with two-point boundary conditions. The arguments are based on the lower and upper solutions method [29,30,31,32,33], which requires a new definition of lower and upper functions to overcome the couple variation on the nonlinearities (see Definition 2.1). A Nagumo condition (see, for example, [34,35,36]) plays an important role to control the first derivatives variation, and the theory of the topological degree (see, for instance, [37,38]) is the main tool to prove the existence of solution for the parameters' values such that there are lower and upper solutions for (E), (B). Therefore, the main result is an existence and localization theorem, as it provides not only the existence of a solution, but also a range where the solution varies.
The paper is organized as follows: Section 2 contains the functional framework, a definition of upper-lower solutions, the Nagumo conditions and "a priori" estimates of the first derivative of the unknown functions. In Section 3 we present an existence and location result and an example to show the applicability of the main theorem. Section 4 applies our main result to a stationary version of the model presented in [39,40] for complex interactions in social media, the mechanisms and dynamics of information diffusion in online social networks.
In this section, some definitions and lemmas will be introduced for the subsequent analysis, we consider the following functional framework.
Let X=C1[0,1] be the usual Banach space equipped with the norm ‖⋅‖C1, defined by
‖ w‖C1:=max{‖ w‖,‖ w′‖}, |
where
‖y1‖:=maxx∈[0,1]|y1(x)|, |
and X2=C1[0,1]×C1[0,1] with the norm
‖ (u,v)‖X2=max{‖ u‖C1,‖ v‖C1}. |
To apply the lower and upper solutions method, depending on the values of the parameters μ and λ, we introduce a new type of lower and upper definition:
Definition 2.1. Let ai,bi,ci,di,Ai,Bi∈R, such that a2i+bi>0, c2i+di>0 and bi,di≥0, for i=1,2.
A pair of functions (γ1,γ2)∈(C2(]0,1[)∩C1([0,1]))2 is a lower solution of problem (E)-(B) if, for all x∈[0,1],
{γ′′1(x)+f(x,γ1(x),γ2(x),γ′1(x),z1)≥μ m(x),∀z1∈R,γ′′2(x)+h(x,γ1(x),γ2(x),y1,γ′2(x))≥λ n(x),∀y1∈R, | (2.1) |
and
a1γ1(0)−b1γ′1(0)≤A1,c1γ1(1)+d1γ′1(1)≤B1,a2γ2(0)−b2γ′2(0)≤A2,c2γ2(1)+d2γ′2(1)≤B2. | (2.2) |
A pair of functions is an upper solution of problem (E)-(B) if the reversed inequalities are verified.
The so-called Nagumo condition establishes an "a priori" estimation for the first derivatives of the solutions of (E), provided that they satisfy adequate bounds, and is adapted here for coupled systems.
Definition 2.2. Let γi(x), Γi(x), i=1,2, be continuous functions such that
γ1(x)≤Γ1(x), γ2(x)≤Γ2(x), ∀x∈[0,1], |
and consider the sets
S={(x,y0,z0,y1,z1)∈[0,1]×R4:γ1(x)≤y0≤Γ1(x), γ2(x)≤z0≤Γ2(x)}. | (S) |
The continuous functions f,h:[0,1]×R4→R satisfy a Nagumo-type condition relative to the intervals [γ1(x),Γ1(x)] and [γ2(x),Γ2(x)], for all x∈[0,1], if there are k1, k2, such that
k1:=max{Γ1(1)−γ1(0),Γ1(0)−γ1(1)}, | (2.3) |
k2:=max{Γ2(1)−γ2(0),Γ2(0)−γ2(1)}, | (2.4) |
and continuous positive functions φ,ψ:[0,+∞)→(0,+∞), verifying
∫+∞k1dsφ(s)=+∞,∫+∞k2dsψ(s)=+∞. | (N1) |
such that
|f(x,y0,z0,y1,z1)|≤φ(|y1|), ∀(x,y0,z0,y1,z1)∈S,|h(x,y0,z0,y1,z1)|≤ψ(|z1|), ∀(x,y0,z0,y1,z1)∈S. | (N2) |
The priori estimates for the first derivatives are given by the next lemma.
Lemma 2.1. Suppose that the continuous functions f,h:[0,1]×R4→R satisfy a Nagumo type condition relative to the intervals [γ1(x),Γ1(x)] and [γ2(x),Γ2(x)], for all x∈[0,1].
Then for every solution (u,v)∈(C2[0,1])2 of (E) verifying
γ1(x)≤u(x)≤Γ1(x)andγ2(x)≤v(x)≤Γ2(x),∀x∈[0,1], | (2.5) |
there are N1,N2>0 (depending only on the parameters μ and λ and the functions m, n, γ1,Γ1,γ2,Γ2,φ and ψ), such that
‖u′‖≤N1and‖v′‖≤N2. | (2.6) |
Proof. Let (u(x),v(x)) be a solution of (E) verifying (2.5). By the Mean Value Theorem, there are x0,x1∈[0,1] such that
u′(x0)=u(1)−u(0)andv′(x1)=v(1)−v(0). | (2.7) |
If
|u′(x)|≤k1, ∀x∈[0,1], |
then it is enough to define N1:=k1 and the proof is complete.
Moreover, the case |u′(x)|>k1, ∀x∈[0,1], is not possible. In fact, if u′(x)>k1, ∀x∈[0,1], we obtain, by (N2), (2.5) and (2.3), the contradiction
u′(x0)=u(1)−u(0)≤Γ1(1)−γ1(0)≤k1. |
If u′(x)<−k1, ∀x∈[0,1], the contradiction is similar.
Consider Ni>ki, for each i=1,2, such that
∫N1k1dsφ(s)+|μ|‖m‖>1,∫N2k2dsψ(s)+|λ|‖n‖>1, | (N) |
and assume that there are x2,x3∈[0,1] with x2<x3, such that
u′(x2)≤k1andu′(x3)>k1. |
By continuity of u′(x), there exists x4∈[x2,x3] such that u′(x4)=k1.
By a convenient change of variable and using (E) and (N2),
∫u′(x3)u′(x4)dsφ(|s|)+|μ|‖m‖=∫x3x4u′′(x)φ(|u′(x)|)+|μ|‖m‖dx≤∫10|u′′(x)|φ(|u′(x)|)+|μ|‖m‖dx≤∫10|μm(x)−f(x,u(x),v(x),u′(x),v′(x))|φ(|u′(x)|)+|μ|‖m‖dx,≤∫10|μ|‖m‖+|f(x,u(x),v(x),u′(x),v′(x))|φ(|u′(x)|)+|μ|‖m‖dx,≤∫10|μ|‖m‖+φ(|u′(x)|)φ(|u′(x)|)+|μ|‖m‖dx=1, |
and by (N)
∫u′(x3)u′(x4)dsφ(|s|)+|μ|‖m‖≤1<∫N1k1dsφ(|s|)+|μ|‖m‖. |
Therefore u′(x3)<N1, and as x3 is taken arbitrarily, then u′(x)<N1, for the values of x whenever u′(x)>k1.
The case for x2>x3 follows similar arguments.
The other possible case where
u′(x2)>−k1andu′(x3)<−k1, |
can be proved by the previous techniques. Therefore ‖u′‖≤N1.
By a similar method, it can be shown that ‖v′‖≤N2.
Remark 2.1. From the previous demonstration, it follows that N1 and N2 can be considered independently of μ and λ, since μ and λ belong to a bounded set.
The first theorem is an existence and localization result:
Theorem 3.1. Let f,h:[0,1]×R4→R be continuous functions. If there are lower and upper solutions of (E)-(B), (γ1,γ2) and (Γ1,Γ2), respectively, according Definition 2.1, such that
γi(x)≤Γi(x),i=1,2,∀x∈[0,1], | (3.1) |
and f and h verify Nagumo conditions as in Definition 2.2, relative to the intervals [γ1(x),Γ1(x)] and [γ2(x),Γ2(x)], for all x∈[0,1], with
f(x,y0,z0,y1,z1)nondecreasinginz0, | (3.2) |
for x∈[0,1], ∀z1∈R,
min{minx∈[0,1]γ′1(x),minx∈[0,1]Γ′1(x)}≤y1≤max{maxx∈[0,1]γ′1(x),maxx∈[0,1]Γ′1(x)}, |
and
h(x,y0,z0,y1,z1)nondecreasinginy0, |
for x∈[0,1], ∀y1∈R,
min{minx∈[0,1]γ′2(x),minx∈[0,1]Γ′2(x)}≤z1≤max{maxx∈[0,1]γ′2(x),maxx∈[0,1]Γ′2(x)}. |
Then there is at least a pair (u(x),v(x))∈(C2[0,1])2 solution of (E)-(B) and, moreover,
γ1(x)≤u(x)≤Γ1(x),γ2(x)≤v(x)≤Γ2(x),∀x∈[0,1]. | (3.3) |
Proof. Define the functions α,β:[0,1]×R→R given by
α(x,y0)={Γ1(x)ify0>Γ1(x)y0ifγ1(x)≤y0≤Γ1(x)γ1(x)ify0<γ1(x) | (3.4) |
and
β(x,z0)={Γ2(x)ifz0>Γ2(x)y1ifγ2(x)≤z0≤Γ2(x)γ2(x)ifz0<γ2(x). | (3.5) |
For θ,ϑ∈[0,1], consider the truncated and perturbed auxiliary problem formed by the equations
{u′′(x)+θ f(x,α(x,u(x)),β(x,v(x)),u′(x),v′(x))=u(x)+θ [μ m(x)−α(x,u(x))]v′′(x)+ϑ h(x,α(x,u(x)),β(x,v(x)),u′(x),v′(x))=v(x)+ϑ [λ n(x)−β(x,v(x))], | (3.6) |
for x∈]0,1[, and the boundary conditions
u(0)=θ [A1−a1α(0,u(0))+b1u′(0)+α(0,u(0))],u(1)=θ [B1−c1α(1,u(1))−d1u′(1)+α(1,u(1))],v(0)=ϑ [A2−a2β(0,v(0))+b2v′(0)+β(0,v(0))],v(1)=ϑ [B2−c2β(1,v(1))−d2v′(1)+β(1,v(1))] | (3.7) |
where ai,bi,ci,di,Ai,Bi∈R, i=1,2, such that a2i+bi>0, c2i+di>0 and bi,di≥0.Take ri>0, i=1,2, such that, ∀x∈[0,1],
−ri<γi(x)≤Γi(x)<ri,μ m(x)−f(x,γ1(x),β(x,v(x)),0,v′(x))−r1−γ1(x)<0,μ m(x)−f(x,Γ1(x),β(x,v(x)),0,v′(x))+r1−Γ1(x)>0,λ n(x)−h(x,α(x,u(x)),γ2(x),u′(x),0)−r2−γ2(x)<0,λn(x)−h(x,α(x,u(x)),Γ2(x),u′(x),0)+r2−Γ2(x)>0, | (3.8) |
and
|Ai−aiΓi(0)+Γi(0)|<ri,|Ai−aiγi(0)+γi(0)|<ri,|Bi−ciΓi(1)+Γi(1)|<ri,|Bi−ciγi(1)+γi(1)|<ri. | (3.9) |
Claim 1. Every solution (u(x),v(x)) of the problems (3.6) and (3.7) verifies
|u(x)|<r1 and |v(x)|<r2, ∀x∈[0,1], |
independently of θ,ϑ∈[0,1] . Assume, by contradiction, that there exist θ∈[0,1], (u(x),v(x)) solution of (3.6) and (3.7) and x∈[0,1] such that |u(x)|≥r1.If u(x)≥r1, define
maxx∈[0,1]u(x):=u(x0). |
For x0∈]0,1[ and θ∈]0,1], u′(x0)=0 and u′′(x0)≤0. By (3.8), we have the following contradiction
0≥u′′(x0)=u(x0)+θ [μ m(x0)−α(x0,u(x0))]−θf(x0,α(x0,u(x0)),β(x0,v(x0)),u′(x0),v′(x0))=u(x0)+θ [μ m(x0)−Γ1(x0)]−θf(x0,Γ1(x0),β(x0,v(x0)),0,v′(x0))≥θ [μ m(x0)−f(x0,Γ1(x0),β(x0,v(x0)),0,v′(x0))+u(x0)−Γ1(x0)]≥θ [μ m(x0)−f(x0,Γ1(x0),β(x0,v(x0)),0,v′(x0))+r1−Γ1(x0)]>0. |
If θ=0, the contradiction arises from
0≥u′′(x0)=u(x0)≥r1>0. |
If x0=0, then
maxx∈[0,1]u(x):=u(0), |
and u′(0+)=u′(0)≤0. By (3.7) and (3.9), we have
r1≤u(0)=θ [A1−a1α(0,u(0))+b1u′(0)+α(0,u(0))]=θ [A1−a1Γ1(0)+b1u′(0)+Γ1(0)]≤θ [A1−a1Γ1(0)+Γ1(0)]≤|A1−a1Γ1(0)+Γ1(0)|<r1. |
If x0=1 a contradiction is obtained analogously.
Then u(x)<r1 for x∈[0,1] and regardless of θ. The other possible case where
u(x)>−r1, for x∈[0,1], |
can be proved by similar techniques.
Therefore |u(x)|<r1 for all x∈[0,1], regardless of θ.
By a similar method, it can be proved that |v(x)|<r2 for all x∈[0,1] regardless of ϑ.
Claim 2. For every solution (u(x),v(x)) of the problems (3.6) and (3.7),
|u′(x)|<N1 and |v′(x)|<N2, ∀x∈[0,1], |
independently of θ,ϑ∈[0,1], with N1 and N2 given by Lemma 2.1.
Define the continuous functions Fθ,Hϑ :[0,1]×R4→R, by
Fθ(x,y0,z0,y1,z1):=θ f(x,α(x,y0),β(x,z0),y1,z1)−y0+θ α(x,y0), |
and
Hϑ(x,y0,z0,y1,z1):=ϑ h(x,α(x,y0),β(x,z0),y1,z1)−z0+ϑ β(x,z0), |
with y0∈[−r1,r1] and z0∈[−r2,r2].
As the functions f,h:[0,1]×R4→R satisfy a Nagumo-type condition relative to the intervals [γ1(x),Γ1(x)] and [γ2(x),Γ2(x)], then
|Fθ(x,y0,z0,y1,z1)|≤|f(x,α(x,y0),β(x,z0),y1,z1)|+|y0|+|α(x,y0)|≤φ(|y1|)+2r1, |
and
|Hϑ(x,y0,z0,y1,z1)|≤|h(x,α(x,y0),β(x,z0),y1,z1)|+|z0|+|β(x,z0)|≤ψ(|z1|)+2r2. |
Therefore for continuous positive functions φ∗,ψ∗:[0,+∞)→(0,+∞), given by
φ∗(|y1|):=φ(|y1|)+2r1andψ∗(|z1|):=ψ(|z1|)+2r2, |
then, clearly, Fθ and Hϑ satisfy Nagumo conditions in the sets
E={(x,y0,z0,y1,z1)∈[0,1]×R4:|y0|≤r1, |z0|≤r2}, |
and, by (N1), we have
∫N1k1dsφ∗(s)=∫N1k1dsφ(s)+2r1>1, |
and
∫N2k2dsψ∗(s)=∫N2k2dsψ(s)+2r2>1. |
Therefore, by Lemma 2.1,
|u′(x)|<N1 and |v′(x)|<N2, ∀x∈[0,1], |
independently of θ,ϑ∈[0,1].
Claim 3. The problems (3.6) and (3.7), for θ=1 and ϑ=1, has at least one solution (u,v).
Define the operators
L:(C2([0,1]))2→(C2([0,1]))2×R4, |
given by
L(u,v)=(u′′−u,v′′−v,u(0),u(1),v(0),v(1)), |
and
N(θ,ϑ):(C1([0,1]))2→(C2([0,1]))2×R4, |
given by
N(θ,ϑ)(u,v)=(X,Y,Aθ,Bθ,Aϑ,Bϑ), |
being
X:=−θ f(x,α(x,u(x)),β(x,v(x)),u′(x),v′(x))+θ [μ m(x)−α(x,u(x))], |
Y:=−ϑ h(x,α(x,u(x)),β(x,v(x)),u′(x),v′(x))+ϑ [λ n(x)−β(x,v(x))], |
Aθ:=θ [A1−a1α(0,u(0))+b1u′(0)+α(0,u(0))],Bθ:=θ [B1−c1α(1,u(1))−d1u′(1)+α(1,u(1))],Aϑ:=ϑ [A2−a2β(0,v(0))+b2v′(0)+β(0,v(0))], |
and
Bϑ:=ϑ [B2−c2β(1,v(1))−d2v′(1)+β(1,v(1))]. |
Since L is invertible, we define the completely continuous operator
T:(C2([0,1]))2→(C2([0,1]))2, |
given by
T(θ,ϑ)(u,v)=L−1N(θ,ϑ)(u,v). |
For M:=max{r1,r2,N1,N2} consider the set
Ω={(u,v)∈C2([0,1]):‖(u,v)‖<M}. |
By Claims 1 and 2, for all θ,ϑ∈[0,1], the degree d(I−T(θ,ϑ),Ω1,0) is well defined, and, by homotopy invariance,
d(I−T(0,0),Ω,0)=d(I−T(1,1),Ω,0). |
As the equation (u,v)=T(0,0)(u,v) admits only the null solution, then, by degree theory,
d(I−T(0,0),Ω,0)=±1, |
and, in particular, the equation (u,v)=T(1,1)(u,v) has at least one solution.
That is, the problem is composed of the equations
{u′′(x)+ f(x,α(x,u(x)),β(x,v(x)),u′(x),v′(x))=u(x)+μ m(x)−α(x,u(x)),v′′(x)+ h(x,α(x,u(x)),β(x,v(x)),u′(x),v′(x))=v(x)+λ n(x)−β(x,v(x)), | (3.10) |
and the boundary conditions
u(0)=A1−a1α(0,u(0))+b1u′(0)+α(0,u(0)),u(1)=B1−c1α(1,u(1))−d1u′(1)+α(1,u(1)),v(0)=A2−a2β(0,v(0))+b2v′(0)+β(0,v(0)),v(1)=B2−c2β(1,v(1))−d2v′(1)+β(1,v(1)) | (3.11) |
has at least one solution (u1(x),v1(x)) in Ω1.
Claim 4. The functions u1(x) and v1(x) are a solution of the initial problem (E), (B).
In fact, if the pair (u1(x),v1(x))∈(C2[0,1])2 is a solution of (3.10) and (3.11), it will be also a solution of the initial problems (E) and (B), provided that
γ1(x)≤u1(x)≤Γ1(x),γ2(x)≤v1(x)≤Γ2(x),∀x∈[0,1]. |
Suppose, by contradiction, that there exists x∈[0,1] such that u1(x)>Γ1(x), and define
maxx∈[0,1][u1(x)−Γ1(x)]:=u1(x1)−Γ1(x1)>0. |
If x1∈]0,1[ then
u′1(x1)=Γ′1(x1)andu′′1(x1)≤Γ′′1(x1), |
and we have, by Definition 2.1, the following contradiction
0≥u′′1(x1)−Γ′′1(x1)=−f(x1,α(x1,u1(x1)),β(x1,v1(x1)),u′1(x1),v′1(x1))+u(x1)+μ m(x1)−α(x1,u1(x1))−Γ′′1(x1)=−f(x1,Γ1(x1),β(x1,v1(x1)),Γ′1(x1),v′1(x1))+u(x1)+μ m(x1)−Γ1(x1)−Γ′′1(x1)≥−f(x1,Γ1(x1),Γ2(x1),Γ′1(x1),v′1(x1))+u(x1)+μ m(x1)−Γ1(x1)−Γ′′1(x1)>−f(x1,Γ1(x1),Γ2(x1),Γ′1(x1),v′1(x1))+μ m(x1)−Γ′′1(x1)≥0. |
For x1=0,
maxx∈[0,1][u1(x)−Γ1(x)]:=u1(0)−Γ1(0)>0 |
and
u′1(0+)−Γ′1(0+)=u′1(0)−Γ′1(0)≤0. |
By the boundary conditions (3.11) and Definition 2.1, this contradiction is obtained
Γ1(0)<u1(0)=A1−a1α(0,u(0))+b1u′(0)+α(0,u(0))=A1−a1Γ1(0)+b1u′(0)+Γ1(0)≤−b1Γ′1(0)+b1u′(0)+Γ1(0)=b1[u′(0)−Γ′1(0)]+Γ1(0)≤Γ1(0). |
So, x1≠0 and by a similar method it is shown that x1≠1. Therefore
u1(x)≤Γ1(x),∀x∈[0,1]. |
Defining
minx∈[0,1][u1(x)−γ1(x)]:=u1(x2)−γ1(x2)<0, |
it can be proved that u1(x)≥γ1(x), for all x∈[0,1], by an analogous process.
Using the same technique, it can be shown that
γ2(x)≤v1(x)≤Γ2(x),∀x∈[0,1]. |
So, (u1(x),v1(x)) is a solution of (E)-(B), for the values of μ,λ∈R, such that there are lower and upper solutions according to Definition 2.1.
Example 3.1. Consider the system
{u′′(x)−sin(π2u(x))+x2v(x)−u′(x)+1v′2(x)+1=μv′′(x)+eu(x)−1−v(x)+cos(π2u′(x))−v′(x)=λ, | (3.12) |
for x∈[0,1], and μ,λ are real parameter, along with boundary conditions
u(0)=0,u(1)+u′(1)=1,v(0)=0,v(1)+v′(1)=1. | (3.13) |
The functions γ1,γ2,Γ1,Γ2:[0,1]→R, given by
γ1(x)=−x, γ2(x)=−x−1,Γ1(x)=x, Γ2(x)=x+1, |
are, respectively, lower and upper solutions of (3.12) and (3.13) for μ and λ such that
μ∈[0,1]andλ∈[1e−1,1e+1]. |
The functions
f(x,y0,z0,y1,z1)=−sin(π2y0)+x2z0−y1+1z21+1 |
and
h(x,y0,z0,y1,z1)=ey0−1−z0+cos(π2y1)−z1 |
are continuous and satisfy the Nagumo conditions (N1) and (N2). By Theorem 3.1, the problems (3.12) and (3.13) has at least one solution (u1(x),v1(x)), which verifies
−x≤u1(x)≤xand−x−1≤v1(x)≤x+1,∀x∈[0,1]. |
Figures 1 and 2 show the admissible region for solution (u1(x),v1(x)).
In [39,40], the authors study the process of disseminating information in social media to obtain, mathematical predictability in news dissemination to increase the efficiency of the distribution of positive information and, at the same time, reduce information unwanted. In short, it is considered a model to describe the flow of information, based on two similar news sources, that spread with logistic growth independently together with an additional effect one over the other.
It is addressed that, for a given piece of information initiated by two specific users called sources, the density of influenced users in the network depends on the distance x to any source. Based on this model we consider the following stationary system
{u′′(x)+r1d1u(x)(1−u(x)K1)+α1d1u(x)v(x)=μ m(x),v′′(x)+r2d2v(x)(1−v(x)K2)+α2d2u(x)v(x)=λ n(x), | (4.1) |
together with the boundary conditions
u(0)−b1u′(0)=1,u′(1)=0,v(0)−b2v′(0)=1,v′(1)=0, | (4.2) |
where bi,di,ri,Ki∈R+ and αi≥0, i=1,2, having the following meaning:
● u and v are the density of information from the different sources
● d1,d2 represent the popularity of the two pieces of information;
● r1,r2 are the speed with which information spreads within groups of users with the same distance;
● K1,K2 represents the carrying capacity, which is the maximum possible density of influenced users;
● α1 measures the positive effect of news v on u and α2 measures the positive effect of news u on v;
● m,n:[0,1]→R+ are continuous functions, μ,λ real parameters, both relating with distance of each source.
● b1, b2 are related with the initial spread of each source.
Define
m≡maxx∈[0,1]m(x)andn≡maxx∈[0,1]n(x), |
consider K1=1 and K2=1, in the sense that the maximum load capacity is 100 and, as a numeric example, assume that
b1∈]0,16], b2∈]0,12],23+11r1144d1+11(4π2−1)α148π2d1<1,18+(4π2−1)r216π4d2+11(4π2−1)α248π2d2<32. |
Then the functions
γ1(x)=34(x−1)2, γ2(x)=12(x−1)2Γ1(x)=112x4−16x2+1, Γ2(x)=14π2cos2(π2x)+(4π2−1)4π2 |
are, respectively, lower and upper solutions of problems (4.1) and (4.2) for
μ∈[1m(23+11r1144d1+11(4π2−1)α148π2d1),1m] | (4.3) |
and
λ∈[1n(18+(4π2−1)r216π4d2+11(4π2−1)α248π2d2),32n]. | (4.4) |
Moreover, the problems (4.1) and (4.2) are particular cases of (E), (B), with
f(x,y0,z0,y1,z1)=r1d1y0(1−y0)+α1d1y0z0, |
and
h(x,y0,z0,y1,z1)=r2d2z0(1−z0)+α2d2y0z0. |
These functions verify the Nagumo conditions (N1) and (N2), relative to the intervals y0∈[γ1(x),Γ1(x)] and z0∈[γ2(x),Γ2(x)], as
|f(x,y0,z0,y1,z1)|=|r1d1y0(1−y0)+α1d1y0z0|≤r1d1|y0(1−y0)|+α1d1|y0z0|≤12d1(12r1+α1), |
|h(x,y0,z0,y1,z1)|=|r2d2z0(1−z0)+α2d2y0z0|≤r2d2|z0(1−z0)|+α2d2|y0z0|≤12d2(12r2+α2). |
and, trivially,
∫+∞ds12di(12ri+αi)=+∞, for i=1,2. |
So by Theorem 3.1 the problems (4.1) and (4.2) have at least one solution (u(x),v(x)), for the values of μ and λ verifying (4.3) and (4.4), such that
34(x−1)2≤u(x)≤112x4−16x2+1, |
and
12(x−1)2≤v(x)≤14π2cos2(π2x)+(4π2−1)4π2, |
for all x∈[0,1].
The Figures 3 and 4 show the regions where this solution lies.
As far as we know, it is the first paper where Ambrosetti-Prodi differential equations are considered in couple systems with different parameters, therefore with present a preliminary study where the solvability of such problems is obtained for parameters' values for which there are lower and upper solutions. There are a lot of open issues such as how the Ambosetti-Prodi alternative could be done for coupled systems, and what are the sufficient conditions on the nonlinearities to discuss the existence, non-existence, and multiplicity of coupled systems solutions
We highlight two aspects in this work:
● A new definition type of lower and upper solutions for coupled systems (see Definition 2.1), which overcomes the nonlinear dependence on the two unknown functions and is will be crucial for future work;
● In the presence of such lower and upper solutions the parameters always belong to bounded sets, as it is illustrated in Example 3.1 and in the application.
The main result allows us to evaluate some parameter values for which there are lower and upper solutions, and, therefore, it shows that, for these values, there is also, at least, a solution and this solution is localized in a strip bounded by lower and upper solutions.
The lower and upper solutions method seems to be a powerful tool to deal with these Amprosetti-Prodi type problems, as it allows not only some estimations on both parameters for which there are solutions of the coupled systems, but also because it provides strips for the localization of such solutions.
In fact, this localization tool, in our opinion, has been undervalued, as it maybe very useful to know some qualitative properties of the unknown functions.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
This research was partially supported by national funds through the Fundação para a Ciência e Tecnologia, FCT, under the project UIDB/04674/2020.
F. Minhós is the Guest Editor of special issue "Boundary Value Problems and Applications" for AIMS Mathematics. F. Minhós was not involved in the editorial review and the decision to publish this article.
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1. | Feliz Minhós, Gracino Rodrigues, Ambrosetti–Prodi Alternative for Coupled and Independent Systems of Second-Order Differential Equations, 2023, 11, 2227-7390, 3645, 10.3390/math11173645 |