The Burgers-KdV equation as a highly nonlinear model, is commonly used in weakly nonlinear analysis to describe small but finite amplitude ion-acoustic waves. In this study, we demonstrate that by considering viscous dissipation, we can derive the Burgers-KdV limit from a one-dimensional plasma system by using the Gardner-Morikawa transformation. This transformation allows us to obtain both homogeneous and inhomogeneous Burgers-KdV equations, which incorporate dissipative and dispersive terms, for the ionic acoustic system. To analyze the remaining system, we employ the energy method in Sobolev spaces to estimate its behavior. As a result, we are able to capture the Burgers-KdV dynamics over a time interval of order O(ε−1), where ε represents a small parameter.
Citation: Rong Rong, Hui Liu. The Burgers-KdV limit in one-dimensional plasma with viscous dissipation: A study of dispersion and dissipation effects[J]. AIMS Mathematics, 2024, 9(1): 1248-1272. doi: 10.3934/math.2024062
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The Burgers-KdV equation as a highly nonlinear model, is commonly used in weakly nonlinear analysis to describe small but finite amplitude ion-acoustic waves. In this study, we demonstrate that by considering viscous dissipation, we can derive the Burgers-KdV limit from a one-dimensional plasma system by using the Gardner-Morikawa transformation. This transformation allows us to obtain both homogeneous and inhomogeneous Burgers-KdV equations, which incorporate dissipative and dispersive terms, for the ionic acoustic system. To analyze the remaining system, we employ the energy method in Sobolev spaces to estimate its behavior. As a result, we are able to capture the Burgers-KdV dynamics over a time interval of order O(ε−1), where ε represents a small parameter.
A century ago, the first metric fixed-point theorem was published by Banach [1]. In fact, before Banach, some famous mathematicians such as Picard and Liouville had used the fixed point approach to solve certain differential equations, more precisely, initial value problems. Inspired by their results, Banach considered it as a separated and independent result in the framework of the nonlinear functional analysis and point-set topology. The statement and the proof of an outstanding work of Banach, also known as contraction mapping principle, can be considered as an art piece: Each contraction, in the setting of a complete metric space, possesses a unique fixed point. Metric fixed point theory has been appreciated and investigated by several researchers. These researchers have different reasons and motivations to study this theory. The most important reason why the researchers find worthful to work and investigate metric fixed point theory is the natural and strong connection of the theoretical result in nonlinear functional analysis with applied sciences. If we look at it with the chronological aspect, we note that the fixed point theory was born as a tool to solve certain differential equations. Banach liberated the theory from being a tool in applied mathematics to an independent work of nonlinear functional analysis. On Picard and Liouville's side, it is a tool to solve the initial value problem. On the other side, from Banach's point of view, the fixed point theory is an independent research topic that has enormous application potential on almost all qualitative sciences, including applied mathematics. Secondly, Banach fixed point theorem not only guarantee the solution (the existence of a fixed point) but also indicate how we reach the mentioned solution (how to find the fixed point). Finally, we need to underline that almost all real world problems can be transferred to a fixed point problem, easily.
With this motivation, several generalizations and extensions of Banach's fixed point theory have been released by introducing new contractions or by changing the structure of the studied abstract space. Among, we shall mention only a few of them that set up the skeleton of the contraction dealt with it. Historically, the first contraction we shall focus on it is the Meir-Keeler contraction [2]. Roughly speaking, the Meir-Keeler contraction can be considered as a uniform contraction. The second contraction that we dealt with is Jaggi contraction [3]. The interesting part of Jaggi's contraction is the following: Jaggi's contraction is one of the first of its kind that involves some rational expression. The last one is called as an interpolative contraction [4]. In the interpolative contraction the terms are used exponentially instead of standard usage of them.
In this paper, we shall introduce a new contraction, hybrid Jaggi-Meir-Keeler type contraction, as a unification and generalization of the Meir-Keeler's contraction, the Jaggi's contraction and interpolative contraction in the setting of a complete metric space. We propose certain assumptions to guarantee the existence of a fixed point for such mappings. In addition, we express some example to indicate the validity of the derived results.
Before going into details, we would like to reach a consensus by explaining the concepts and notations: Throughout the paper, we presume the sets, we deal with, are non-empty. The letter N presents the set of positive integers. Further, we assume that the pair (X,d) is a complete metric space. This notation is required in each of the following theorems, definitions, lemma and so on. We shall use the pair (X,d) everywhere without repeating that it is a complete metric space.
In what follows we recall the notion of the uniform contraction which is also known as Meir-Keeler contraction:
Definition 1.1. [2] A mapping f:(X,d)→(X,d) is said to be a Meir-Keeler contraction on X, if for every E>0, there exists δ>0 such that
E≤d(x,y)<E+δimpliesd(fx,fy)<E, | (1.1) |
for every x,y∈X.
Theorem 1.1. [2] Any Meir-Keeler contraction f:(X,d)→(X,d) possesses a unique fixed point.
Very recently, Bisht and Rakočević [5] suggested the following extension of the uniform contraction:
Theorem 1.2. [5] Suppose a mapping f:(X,d)→(X,d) fulfills the following statements:
(1) for a given E>0 there exists a δ(E)>0 such that
E<M(x,y)<E+δ(E)impliesd(fx,fy)≤E; |
(2) d(fx,fy)<M(x,y), whenever M(x,y)>0;
for any x,y∈X, where
M(x,y)=max{d(x,y),αd(x,fx)+(1−α)d(y,fy),(1−α)d(x,fx)+αd(y,fy),β[d(x,fy)+d(y,fx)]2}, |
with 0<α<1,0≤β<1.Then, f has a unique fixed point u∈X and fnx→u for each x∈X.
On the other hand, in 2018, the idea of interpolative contraction was consider to revisit the well-known Kannan's fixed point theorem [6]:
Definition 1.2. [4] A mapping f:(X,d)→(X,d) is said to be an interpolative Kannan type contraction on X if there exist κ∈[0,1) and γ∈(0,1) such that
d(fx,fy)≤κ[d(x,fx)]γ[d(y,fy)]1−γ, | (1.2) |
for every x,y∈X∖Fix(f), where Fix(f)={x∈X|fx=x}.
Theorem 1.3. [4] Any interpolative Kannan-contraction mapping f:(X,d)→(X,d) possesses a fixed point.
For more interpolative contractions results, we refer to [7,8,9,10,11] and related references therein.
Definition 1.3. A mapping f:(X,d)→(X,d) is called a Jaggi type hybrid contraction if there is ψ∈Ψ so that
d(fx,fy)≤ψ(Jsf(x,y)), | (1.3) |
for all distinct x,y∈X where p≥0 and σi≥0,i=1,2,3,4, such that σ1+σ2=1 and
Jsf(x,y)={[σ1(d(x,fx)⋅d(y,fy)d(x,y))s+σ2(d(x,y))s]1/p,ifp>0,x,y∈X,x≠y(d(x,fx))σ1(d(y,fy))σ2,ifp=0,x,y∈X∖Ff(X), | (1.4) |
where Ff(X)={z∈X:fz=z}.
Theorem 1.4. A continuous mapping f:(X,d)→(X,d) possesses a fixed point x if it forms a Jaggi-type hybrid contraction.In particular, for any x0∈X, the sequence {fnx0} converges to x.
Definition 1.4. [12] Let α:X×X→[0,+∞) be a mapping, where X≠∅. A self-mapping f:(X,d)→(X,d) is called triangular α-orbital admissible and denote as f∈TαX if
α(x,fx)≥1impliesα(fx,f2x)≥1, |
and
α(x,y)≥1,andα(y,fy)≥1,impliesα(x,fy)≥1 |
for all x,y∈X.
This concept, was used by many authors, in order to prove variant fixed point results (see, for instance [13,14,15,16,17,18,19] and the corresponding references therein).
Lemma 1.1. [12] Assume that f∈TαX. If there exists x0∈X such that α(x0,fx0)≥1, then α(xm,xk)≥1, for all m,n∈N, where the sequence {xk} is defined by xk+1=xk.
The following condition is frequently considered to avoid the continuity of the mappings involved.
(R) if the sequence {xn} in X is such that for each n∈N,
α(xn,xn+1)≥1andlimn→+∞xn=x∈x, |
then there exists a subsequence {xn(j)} of {xn} such that
α(xn(j),x)≥1, for each j∈N. |
We start this section by introducing the new contraction, namely, hybrid Jaggi-Meir-Keeler type contraction.
Consider the mapping f:(X,d)→(X,d) and the set of fixed point, Ff(X)={z∈X:fz=z}. We define the crucial expression Rsf as follows:
Rsf(x,y)={[β1(d(x,fx)⋅d(y,fy)d(x,y))s+β2(d(x,y))s+β3(d(x,fy)+d(y,fx)4)s]1/s,fors>0,x,y∈X,x≠y(d(x,fx))β1(d(y,fy))β2(d(x,fy)+d(y,fx)4)β3,fors=0,x,y∈X, | (2.1) |
where p≥1 and βi≥0, i=1,2,3 are such that β1+β2+β3=1.
Definition 2.1. Assume that f∈TαX. We say that f:(X,d)→(X,d) is an α-hybrid Jaggi-Meir-Keeler type contraction on X, if for all distinct x,y∈X we have:
(a1) for given E>0, there exists δ>0 such that
E<max{d(x,y),Rsf(x,y)}<E+δ⟹α(x,y)d(fx,fy)≤E; | (2.2) |
(a2)
α(x,y)d(fx,fy)<max{d(x,y),Rsf(x,y)}. | (2.3) |
Theorem 2.1. Any continuous α-hybrid Jaggi-Meir-Keeler type contraction f:(X,d)→(X,d) provide a fixed point if there exists x0∈X, such that α(x0,fx0)≥1 and α(x0,f2x0)≥1.
Proof. Let x0∈X be an arbitrary, but fixed point. We form the sequence {xm}, as follows:
xm=fxm−1=fmx0, |
for all m∈N and assume that d(xm,xm+1)>0, for all n∈N∪{0}. Indeed, if for some l0∈N∪{0} we have d(xl0,xl0+1)=0, it follows that xl0=xl0+1=fxl0. Therefore, xl0 is a fixed point of the mapping f and the proof is closed.
Since, by assumption, the mapping f is triangular α-orbital admissible, it follows that
α(x0,fx0)≥1⇒α(x1,x2)=α(fx0,f2x0)≥1⇒...⇒ |
α(xn,xn+1)≥1, | (2.4) |
for every n∈N.
We shall study two cases; these are s>0 and s=0.
Case (A). For the case s>0, letting x=xn−1 and y=xn=fxn−1 in (a2), we get
d(xn,xn+1)≤α(xn−1,xn)d(fxn−1,fxn)<max{d(xn−1,xn),Rsf(xn−1,xn)}, | (2.5) |
where
Rsf(xn−1,xn)=[β1(d(xn−1,fxn−1)⋅d(xn,fxn)d(xn−1,xn))s+β2(d(xn−1,xn))s++β3(d(xn−1,fxn)+d(xn,fxn−1)4)s]1/s=[β1(d(xn−1,xn)⋅d(xn,xn+1)d(xn−1,xn))s+β2(d(xn−1,xn))s++β3(d(xn−1,xn+1)+d(xn,xn)4)s]1/s≤[β1(d(xn,xn+1))s+β2(d(xn−1,xn))s++β3(d(xn−1,xn)+d(xn,xn+1)4)s]1/s. |
If we can find n0∈N such that d(xn0,xn0+1)≥d(xn0−1,xn0), we have
Rsf(xn0−1,xn0)≤[β1(d(xn0,xn0+1))s+β2(d(xn0,xn0+1))s++β3(d(xn0,xn0+1))s]1/s=d(xn0,xn0+1)(β1+β2+β3)1/s=d(xn0,xn0+1). |
Then, max{d(xn0,xn0+1),Rsf(xn0−1,xn0)}=d(xn0,xn0+1), and using (2.4), respectively (2.5) we get
d(xn0,xn0+1)≤α(xn0−1,xn0)d(fxn+0−1,fxn0)<max{d(xn0,xn0+1),Rsf(xn0−1,xn0)}≤d(xn0,xn0+1), |
which is a contradiction. Therefore, d(xn,xn+1)<d(xn−1,xn) for all n∈N and (2.5) becomes
d(xn,xn+1)<d(xn−1,xn), |
for all n∈N. Consequently, there exists b≥0 such that limn→+∞d(xn−1,xn)=b. If b>0, we have
d(xm,xm+1)≥b>0, |
for any m∈N. On the one hand, since (2.2) holds for every given E>0, it is possible to choose E=b and let δ>0 be such that (2.2) is satisfied. On the other hand, since, also, limn→+∞max{d(xn−1,xn),Rsf(xn−1,xn)}=b, there exists m0∈N such that
b<max{d(xm0−1,xm0),Rsf(xm0−1,xm0)}<b+δ. |
Thus, by (2.2), together with (2.4) we obtain
d(xm0,xm0+1)≤α(xm0,xm0+1)d(fxm0−1,fxm0)<b, |
which is a contradiction. Therefore,
limn→+∞d(xn,xn+1)=b=0. | (2.6) |
We claim now that {xn} is a Cauchy sequence. Let E>0 be fixed and we can choose that δ′=min{δ(E),E,1}. Thus, from (2.6) it follows that there exists j0∈N such that
d(xn,xn+1)<δ′2, | (2.7) |
for all n≥j0. Now, we consider the set
A={xl|l≥j0,d(xl,xj0)<E+δ′2}. | (2.8) |
We claim that fy∈A whenever y=xl∈A. Indeed, in case of l=j0, we have fxl=fxj0=xj0+1, and taking (2.7) into account, we get
d(xj0,xj0+1)<δ′2<E+δ′2. | (2.9) |
Thus, we will assume that l>j0, and we distinguish two cases, namely:
Case 1. Suppose that
E<d(xl,xj0)<E+δ′2. | (2.10) |
We have
Rsf(xl,xj0)=[β1(d(xl,fxl)d(xj0,fxj0)d(xl,xj0))s+β2(d(xl,xj0))s+β3(d(xl,fxj0)+d(xj0,fxl)4)s]1/s=[β1(d(xl,xl+1)d(xj0,xj0+1)d(xl,xj0))s+β2(d(xl,xj0))s++β3(d(xl,xj0+1)+d(xj0,xl+1)4)s]1/s≤[β1(d(xl,xl+1)d(xj0,xj0+1)d(xl,xj0))s+β2(d(xl,xj0))s++β3(d(xl,xj0)+d(xj0,xj0+1)+d(xl,xj0)+d(xl,xl+1)4)s]1/s<[β1(d(xl,xl+1))s+β2(d(xl,xj0))s+β3(2d(xl,xj0)+d(xj0,xj0+1)+d(xl,xl+1)4)s]1/s<[β1(δ′2)s+β2(E+δ′2)s+β3(E2+δ′4+δ′4)s]1/s≤(β1+β2+β3)1/s(E+δ′2)≤E+δ′. |
In this case,
E<d(xl,xj0)≤max{d(xl,xj0),Rsf(xl,xj0)}<max{(E+δ′2),(E+δ′)}=(E+δ′), |
which implies by (a1) that
α(xl,xj0)d(fxl,fxj0)≤E. | (2.11) |
But, taking into account that the mapping f is triangular α-orbital admissible, together with (2.4) we have
α(xn,xn+1)≥1 and α(xn+1,fxn+1)≥1 implies α(xn,xn+2)≥1, |
and recursively we get that
α(xn,xl)≥1, | (2.12) |
for all n,l∈N. Therefore, from (2.11) and (2.12), we have
d(xl+1,xj0+1)=d(fxl,fxj0)≤E. | (2.13) |
Now, by the triangle inequality together with (2.7)and (2.13) we get
d(xl+1,xj0)≤d(xl+1,xj0+1)+d(xj0+1,xj0)<(E+δ′2), |
which means that, indeed fxl=xl+1∈A.
Case 2. Suppose that
d(xl,xj0)≤E. | (2.14) |
Thus,
d(fxl,xj0)≤d(fxl,fxj0)+d(fxj0,xj0)≤α(xl,xj0)d(fxl,fxj0)+d(xj0+1,xj0)<max{d(xl,xj0),Rsf(xl,xj0)}+d(xj0+1,xj0), | (2.15) |
where
Rsf(xl,xj0)=[β1(d(xl,xl+1)d(xj0,xj0+1)d(xl,xj0))s+β2(d(xl,xj0))s++β3(d(xl,xj0)+d(xj0,xj0+1)+d(xl,xj0)+d(xl,xl+1)4)s]1/s. |
We must consider two subcases
(2a). d(xl,xj0)≥d(xj0,xj0+1). Then,
Rsf(xl,xj0)≤[β1(d(xl,xl+1))s+β2(d(xl,xj0))s++β3(2d(xl,xj0)+d(xj0,xj0+1)+d(xl,xl+1)4)s]1/s<[β1(δ′2)s+β2(E))s+β3(2E+2δ′24))s]1/s<[β1+β2+β3]1/s(E2+δ′4). |
But, since δ′=min{δ,E,1}, we get
Rsf(xl,xj0)<3E4, |
and then
d(fxl,xj0)<max{d(xl,xj0),Rsf(xl,xj0)}+d(xj0+1,xj0)<max{E,3E4}+δ′2=(E+δ′2), |
which shows that fxl∈A.
(2b). d(xl,xj0)<d(xj0,xj0+1). Then,
d(fxl,xj0)≤xl+1,xl)+d(xl,xj0)<δ′2+δ′2<E+δ′2. |
Consequently, choosing some m,n∈N such that m>n>j0, we can write
d(xm,xn)≤d(xm,xj0)+d(xj0,xn)<2(E+δ′2)<4E, |
which leads us to
limm,n→+∞d(xm,xn)=0. |
Therefore, {xm} is a Cauchy sequence in a complete metric space. Thus, we can find a point u∈X such that limm→+∞xm=u. Moreover, since the mapping f is continuous we have
u=limm→+∞fm+1x0=limm→+∞f(fmx0)=f(limm→+∞fmx0)=fu, |
that is, u is a fixed point of f.
Case (B). For the case s=0, letting x=xn−1 and y=xn=fxn−1 in (2.2), we get
d(xn,xn+1)≤α(xn−1,xn)d(fxn−1,fxn)<max{d(xn−1,xn),Rf(xn−1,xn)}, | (2.16) |
where
Rf(xn−1,xn)=[d(xn−1,fxn−1)]β1[d(xn,fxn)]β2[d(xn−1,fxn)+d(xn,fxn−14]β3=[d(xn−1,xn)]β1[d(xn,xn+1)]β2[d(xn−1,xn+1)+d(xn,xn4]β3=[d(xn−1,xn)]β1[d(xn,xn+1)]β2[d(xn−1,xn+1)+d(xn,xn4]β3≤[d(xn−1,xn)]β1[d(xn,xn+1)]β2[d(xn−1,xn)+d(xn,xn+1)4]β3=[d(xn−1,xn)]β1[d(xn,xn+1)]β2[d(xn−1,xn)+d(xn,xn+1)4]β3 |
Thus, by (2.3) and taking (2.4) into account we have
d(xn,xn+1)≤α(xn−1,xn)d(fxn−1,fxn)<max{d(xn−1,xn),Rf(xn−1,xn)}. |
Now, if there exists n0∈N such that d(xn0,xn0+1)≥d(xn0−1,xn0), we get
d(xn0,xn0+1)<max{d(xn0−1,xn0),Rf(xn0−1,xn0)}≤max{d(xn0−1,xn0),d(xn0,xn0+1)}<d(xn0,xn0+1), |
which is a contradiction. Therefore, d(xn,xn+1)<d(xn−1,xn) for all n∈N, that is, the sequence {xn} decreasing and moreover, converges to some b≥0. Moreover, since
Rf(xn−1,xn)=[d(xn−1,xn)]β1[d(xn,xn+1)]β2[d(xn−1,xn+1)4]β3, |
we get that
limn→+∞max{d(xn−1,xn),Rf(xn−1,xn)}=b. |
If we suppose that b>0, then, 0<b<d(xn−1,xn) and we can find δ>0 such that
b<max{d(xn−1,xn),Rf(xn−1,xn)}<b+δ. |
In this way, taking E=b, we get
b=E<max{d(xn−1,xn),Rf(xn−1,xn)}<E+δ, |
which implies (by (a1)) that
d(xn−1,xn)≤α(xn−1,xn)d(fxn−1,fxn))≤E=b, |
which is a contradiction. We thus proved that
limm→d(xn−1,xn)=0. | (2.17) |
We claim now, that the sequence {xn} is Cauchy. Firstly, we remark that, since d(xn−1,xn)=0, there exists j0∈N, such that
d(xn−1,xn)<δ′2, | (2.18) |
for any n≥j0, where δ′=min{δ,E,1}. Reasoning by induction, we will prove that the following relation
d(xj0,xj0+m)<E+δ′2 | (2.19) |
holds, for any m∈N. Indeed, in case of m=1,
d(xj0,xj0+1)<δ′2<E+δ′2, |
so, (2.19) is true. Now, supposing that (2.19) holds for some l, we shall show that it holds for l+1. We have
Rf(xj0,xj0+l)=(d(xj0,fxj0))β1(xj0+l,fxj0+l)s(d(xj0,fxj0+l)+d(xj0+l,fxj0)4)β3=(d(xj0,xj0+1))β1(xj0+l,xj0+l+1)s(d(xj0,xj0+l+1)+d(xj0+l,xj0+1)4)β3≤(d(xj0,xj0+1))β1(d(xj0+l,xj0+l+1))s(d(xj0,xj0+l)+d(xj0+l,xj0+l+1)+d(xj0+l,xj0)+d(xj0,xj0+1)4)β3<(δ′2)β1+β2((E2+δ′4)+δ′4)β3≤(E+δ′2). | (2.20) |
As in the Case (A), if d(xj0,xj0+l)>E, by (a2), and keeping in mind the above inequalities, we get
E<d(xj0,xj0+l)≤max{d(xj0,xj0+l),Rf(xj0,xj0+l)}<max{δ′2,(E+δ′2)}=E+δ′ implies α(xj0,xj0+l)d(fxj0,fxj0+l)≤E. |
But, since using (2.12), it follows that
d(xj0+1,xj0+l+1)=d(fxj0,fxj0+l)≤E, |
and then, by (b3) we get
d(xj0,xj0+l+1)≤d(xj0,xj0+1)+d(xj0+1,xj0+l+1)<δ′2+E<E+δ′2. |
Therefore, (2.19) holds for (l+1). In the opposite situation, if d(xj0,xj0+l)≤E, again by the triangle inequality, we obtain
d(xj0,xj0+l+1)≤d(xj0,xj0+1)+d(xj0+1,xj0+l+1)≤d(xj0,xj0+1)+α(xj0,xj0+l)d(fxj0,fxj0+l)<δ′2+max{d(xj0,xj0+l),Rf(xj0,xl)}<δ′2+max{E,E2+δ′4}=δ′2+E. |
Consequently, the induction is completed. Therefore, {xm} is a Cauchy sequence in a complete metric space. Thus, there exists u∈X such that fu=u.
In the above Theorem, the continuity condition of the mapping f can be replace by the continuity of f2.
Theorem 2.2. Suppose that f:(X,d)→(X,d) forms an α-hybrid Jaggi-Meir-Keeler type contraction such that f2 is continuous.Then, f has a fixed point, provided that there exists x0∈X, such that α(x0,fx0)≥1.
Proof. Let x0∈X such that α(x0,fx0)≥1 and the sequence {xn}, where xn=fxn−1, for any n∈N. Thus, from Theorem 2.3 we know that this is a convergent sequence. Letting u=limn→+∞xn, we claim that u=fu.
Since the mapping f2 is supposed to be continuous,
f2u=limn→+∞f2xn=u. |
Assuming on the contrary, that u≠fu, we have
Rsf(u,fu)={[β1(d(u,fu)⋅d(fu,f2u)d(u,fu))s+β2(d(u,fu))s+β3(d(u,f2u)+d(fu,fu)4)s]1/s,fors>0(d(u,fu))β1(d(fu,f2u))β2(d(u,f2u)+d(fu,fu)4)β3,fors=0[16pt]={[β1(d(u,fu)⋅d(fu,u)d(u,fu))s+β2(d(u,fu))s+β3(d(u,u)+d(fu,fu)4)s]1/s,fors>0(d(u,fu))β1(d(fu,u))β2(d(u,u)+d(fu,fu)4)β3,fors=0[16pt]={[β1(d(fu,u))s+β2(d(u,fu))s]1/s,fors>00,fors=0={[β1+β2]1/sd(u,fu)),fors>00,fors=0 |
Example 2.1. Let X=[0,+∞), d:X×X→[0,+∞), d(x,y)=|x−y|, and the mapping f:X→X, where
f={12,ifx∈[0,1]16,ifx>1. |
We can easily observe that f is discontinuous at the point x=1, but f2 is a continuous mapping. Let also the function α:X×X→[0,+∞),
α(x,y)={x2+y2+1,ifx,y∈[0,1]ln(x+y)+1,ifx,y∈(1,+∞)1,ifx=56,y=760, otherwise , |
and we choose β1=14,β2=12,β1=14 and s=2. The mapping f is triangular α-orbital admissible and satisfies (a2) in Definition 2.1 for any x,y∈[0,1], respectively for x,y∈(1,+∞). Taking into account the definition of the function α, we have more to check the case x=56, y=76. We have
Rf(56,76)=[14(d(56,f56)d(76,f76)d(56,76))2+12(d(56,76))2+14(d(56,f76)+d(76,f56)4)2]1/2=√14+12⋅19+19⋅=√13. |
Therefore,
α(56,76)d(f56,f76)=d(f56,f76)=d(12,16)=13<1√3=max{d(56,76),Rf(56,76)}. |
Moreover, since the mapping f satisfies condition (a1) for
δ(E)={1−E,forE<11,forE≥1, |
it follows that the assumptions of Theorem 2.3 are satisfied, and u=12 ia a fixed point of the mapping f.
Theorem 2.3. If to the hypotheses of Theorem we add the following assumption
α(u,v)≥1for anyu,v∈Ff(X), |
then the mapping f admits an unique fixed point.
Proof. Let u∈X be a fixed point of f. Supposing on the contrary, that we can find v∈X such that fu=u≠v=fv, we have
(i) For s>0,
Rsf=[β1(d(u,fu)d(v,fv)d(u,v))s+β2(d(u,v))s+β3(d(u,fv)+d(v,fu)4)s]1/s=[β2(d(u,v))s+β3(d(u,v)2)s]1/s≤(β2+β3)1/sd(u,v)≤d(u,v). |
Thus, taking x=u and y=v in (2.3) we get
d(u,v)≤α(u,v)d(fu,fv)<max{d(u,v),Rf(u,v)}=d(u,v), |
which is a contradiction.
(ii) For s=0,
d(u,v)≤α(u,v)d(fu,fv)<max{d(u,v),Rf(u,v)}=max{d(u,v),(d(u,fu))β1(d(v,fv))β2(d(u,fv)+d(v,fu)4)β3}=d(u,v), |
which is a contradiction.
Consequently, if there exists a fixed point of the mapping f, under the assumptions of the theorem, this is unique.
Example 2.2. Let the set X=[−1,+∞), d:X×X→[0,+∞), d(x,y)=|x−y|, and the mapping f:X→X, where
fx={x2+1,ifx∈[−1,0)1,ifx∈[0,1]1x,ifx>1. |
Let also α:X×X→[0,+∞) defined as follows
α(x,y)={34,ifx,y∈[−1,0)x2+y2+1,ifx,y∈[0,1]1,ifx∈[−1,0),y∈[0,1]0, otherwise . |
It is easy to check that, with these chooses, f is a continuous triangular α-orbital admissible mapping and also, it follows that the mapping f satisfies the conditions (a2) from Definition (2.1). Moreover, f satisfies the condition (a1), considering δ(E)=1−E in case of E<1 and δ(E)=1 for E≥1. Consequently, f satisfies the conditions of Theorem 2.3 and has a unique fixed point, u=0.
In particular, for the case s=0, the continuity assumption of the mapping f can be replace by the condition (R).
Theorem 2.4. We presume thatf:(X,d)→(X,d)∈TαX and fulfills
(ai) for given E>0, there exists δ>0 such that
E<O(x,y)<E+δimpliesα(x,y)d(fx,fy)≤E, | (2.21) |
with
O(x,y)=max{d(x,y),(d(x,fx))β1(d(y,fy))β2(d(x,fy)+d(y,fx)4)β3}, |
for all x,y∈X, where βi≥0, i=1,2,3 so that β1+β2+β3=1;
(aii)
α(x,y)d(fx,fy)<O(x,y). | (2.22) |
The mapping f has a unique fixed point provided that:
(α1) there exists x0∈X such that α(x0,fx0)≥1;
(α3) α(u,v)≥1 for any u,v∈Ff(X);
(α2) if the sequence {xn} in X is such that for each n∈N
α(xn,xn+1)≥1andlimn→+∞xn=x∈X, |
then there exists a subsequence {xn(j)} of {xn} such that
α(xn(j),x)≥1,for eachj∈N. |
Proof. Let x0∈X such that α(x0,fx0)≥1. Then, we know (following the proof of Theorem 2.3) that the sequence {xn}, with xn=fnx0 is convergent; let u=limn→+∞xn. On the other hand, from (α2), we can find a subsequence {xn(j)} of {xn} such that
α(xn(j),u)≥1, for each j∈N. |
Since we can suppose that d(xn(j)+1,fu)>0, from (aii) we have
d((xn(j)+1,fu))≤α(xn(j),u)d(fxn(j),fu)<O(x,y)=max{d(xn(j),u),(d(xn(j),fxn(j)))β1(d(u,fu))β2(d(xn(j),fu)+d(u,fxn(j))4)β3}=max{d(xn(j),u),(d(xn(j),xn(j)+1))β1(d(u,fu))β2(d(xn(j),fu)+d(u,xn(j)+1)4)β3}. |
Letting n→+∞ in the above inequality, we get d(u,fu)=0. Thus, fu=u.
To proof the uniqueness, we consider that we can find another fixed point of f. From (aii), we have
d(u,v)=d(fu,fv)≤α(u,v)d(fu,fv)<O(u,v)=d(u,v)<d(u,v), |
which is a contradiction. Therefore, u=v.
Considering α(x,y)=1 in the above theorems, we can easily obtain the following result.
Definition 2.2. A mapping f:(X,d)→(X,d) is called hybrid Jaggi-Meir-Keeler type contraction on X if for all distinct x,y∈X we have:
(a1) for given E>0, there exists δ>0 such that
E<max{d(x,y),Rsf(x,y)}<E+δ⟹d(fx,fy)≤E; | (2.23) |
(a2) whenever Rf(x,y)>0,
d(fx,fy)<max{d(x,y),Rsf(x,y)}. | (2.24) |
Corollary 2.1. Any hybrid Jaggi-Meir-Keeler type contraction f:(X,d)→(X,d) possesses a unique fixed point provided that f is continuous or f2 is continuous.
The authors declare that they have no conflicts of interest.
[1] |
M. Qayyum, E. Ahmad, S. Afzal, S. Acharya, Soliton solutions of generalized third order time-fractional KdV models using extended He-Laplace algorithm, Complexity, 2022 (2022), 2174806. https://doi.org/10.1155/2022/2174806 doi: 10.1155/2022/2174806
![]() |
[2] |
D. Benney, Long waves on liquid films, J. Math. Phys., 45 (1966), 150–155. https://doi.org/10.1002/sapm1966451150 doi: 10.1002/sapm1966451150
![]() |
[3] |
R. Johnson, Shallow water waves on a viscous fluid the undular bore, Phys. Fluids, 15 (1972) 1693–1699. https://doi.org/10.1063/1.1693764 doi: 10.1063/1.1693764
![]() |
[4] | L. Wijngaarden, On the motion of gas bubbles in a perfect fluid, Arch. Mech., 34 (1982), 343–349. |
[5] |
R. Johnson, A nonlinear equation incorporating damping and dispersion, J. Fluid Mech., 42 (1970) 49–60. https://doi.org/10.1017/S0022112070001064 doi: 10.1017/S0022112070001064
![]() |
[6] |
T. Yatabe, T. Kanagawa, T. Ayukai, Theoretical elucidation of effect of drag force and translation of bubble on weakly nonlinear pressure waves in bubbly flows, Phys. Fluids, 33 (2021), 033315. https://doi.org/10.1063/5.0033614 doi: 10.1063/5.0033614
![]() |
[7] | J. Burgers, Mathematical examples illustrating relations occurring in the theory of turbulent fluid motion, In: Selected papers of JM Burgers, Dordrecht: Springer, 1995. https://doi.org/10.1007/978-94-011-0195-0_10 |
[8] |
D. Korteweg, G. de Vries, On the change of form of long waves advancing in a rectangular channel, and on a new type of long stationary waves, The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science, 39 (1895), 422–443. https://doi.org/10.1080/14786449508620739 doi: 10.1080/14786449508620739
![]() |
[9] |
D. Gao, Nonplanar ion acoustic solitary waves in an electronegative plasma by damped Korteweg-de Vries-Burgers equation, Chinese J. Phys., 77 (2022), 1789–1795. https://doi.org/10.1016/j.cjph.2021.11.005 doi: 10.1016/j.cjph.2021.11.005
![]() |
[10] |
N. Cao, X. Yin, S. Bai, L. Xu, Breather wave, lump type and interaction solutions for a high dimensional evolution model, Chaos Soliton. Fract., 172 (2023), 113505. https://doi.org/10.1016/j.chaos.2023.113505 doi: 10.1016/j.chaos.2023.113505
![]() |
[11] |
B. Chentouf, A. Guesmia, Well-posedness and stability results for the Korteweg-de Vries-Burgers and Kuramoto-Sivashinsky equations with infinite memory: A history approach, Nonlinear Anal. Real, 65 (2022), 103508. https://doi.org/10.1016/j.nonrwa.2022.103508 doi: 10.1016/j.nonrwa.2022.103508
![]() |
[12] |
J. Li, K. Liu, Well-posedness of Korteweg-de Vries-Burgers equation on a finite domain, Indian J. Pure Appl. Math., 48 (2017), 91–116. https://doi.org/10.1007/s13226-016-0210-7 doi: 10.1007/s13226-016-0210-7
![]() |
[13] |
R. Duan, H. Zhao, Global stability of strong rarefaction waves for the generalized KdV-Burgers equation, Nonlinear Anal. Theor., 66 (2007), 1100–1117. https://doi.org/10.1016/j.na.2006.01.008 doi: 10.1016/j.na.2006.01.008
![]() |
[14] |
S. EI-Tantawy, A. Salas, M. Alharthi, On the analytical and numerical solutions of the damped nonplanar Shamel Korteweg-de Vries Burgers equation for modeling nonlinear structures in strongly coupled dusty plasmas: Multistage homotopy perturbation method, Phys. Fluids, 33 (2021), 043106. https://doi.org/10.1063/5.0040886 doi: 10.1063/5.0040886
![]() |
[15] |
S. Ivanov, A. Kamchatnov, Formation of dispersive shock waves in evolution of a two-temperature collisionless plasma, Phys. Fluids, 32 (2020), 126115. https://doi.org/10.1063/5.0033455 doi: 10.1063/5.0033455
![]() |
[16] |
L. Molinet, F. Ribaud, On the low regularity of the Korteweg-de Vries-Burgers equation, Int. Math. Res. Notices, 2002 (2002), 1979–2005. https://doi.org/10.1155/S1073792802112104 doi: 10.1155/S1073792802112104
![]() |
[17] |
T. Dlotko, The generalized Korteweg-de Vries-Burgers equation in H2(R), Nonlinear Anal. Theor., 74 (2011), 721–732. https://doi.org/10.1016/j.na.2010.08.043 doi: 10.1016/j.na.2010.08.043
![]() |
[18] |
X. Wang, Z. Feng, L. Debnath, D. Y. Gao, The Korteweg-de Vries-Burgers equation and its approximate solution, Int. J. Comput. Math., 85 (2008), 853–863. https://doi.org/10.1080/00207160701411152 doi: 10.1080/00207160701411152
![]() |
[19] |
Z. Feng, R. Knobel, Traveling waves to a Burgers-Korteweg-de Vries-type equation with higher-order nonlinearities, J. Math. Anal. Appl., 328 (2007), 1435–1450. https://doi.org/10.1016/j.jmaa.2006.05.085 doi: 10.1016/j.jmaa.2006.05.085
![]() |
[20] |
Z. Zhao, L. He, Multiple lump molecules and interaction solutions of the Kadomtsev-Petviashvili I equation, Commun. Theor. Phys., 74 (2022), 105004. https://doi.org/10.1088/1572-9494/ac839c doi: 10.1088/1572-9494/ac839c
![]() |
[21] |
Z. Zhao, L. He, A. Wazwaz, Dynamics of lump chains for the BKP equation describing propagation of nonlinear waves, Chinese Phys. B, 32 (2023), 040501. https://doi.org/10.1088/1674-1056/acb0c1 doi: 10.1088/1674-1056/acb0c1
![]() |
[22] |
Z. Zhao, C. Zhang, Y. Fen, J. Yue, Space-curved resonant solitons and interaction solutions of the (2+1)-dimensional Ito equation, Appl. Math. Lett., 146 (2023), 108799. https://doi.org/10.1016/j.aml.2023.108799 doi: 10.1016/j.aml.2023.108799
![]() |
[23] |
Y. Guo, X. Pu, KdV limit of the Euler-Poisson system, Arch. Rational Mech. Anal., 211 (2014), 673–710. https://doi.org/10.1007/s00205-013-0683-z doi: 10.1007/s00205-013-0683-z
![]() |
[24] |
S. Bai, X. Yin, N. Cao, L. Xu, A high dimensional evolution model and its rogue wave solution, breather solution and mixed solutions, Nonlinear Dyn., 111 (2023), 12479–12494. https://doi.org/10.1007/s11071-023-08467-x doi: 10.1007/s11071-023-08467-x
![]() |
[25] |
X. Pu, Dispersive limit of the Euler-Poisson system in higher dimensions, SIAM J. Math. Anal., 45 (2013), 834–878. https://doi.org/10.48550/arXiv.1204.5435 doi: 10.48550/arXiv.1204.5435
![]() |
[26] |
X. Pu, R. Rong, Zakharov-Kuznetsov-type limit for ion dynamics system with external magnetic field in R3, Appl. Math. Lett., 115 (2020), 106938. https://doi.org/10.1016/j.aml.2020.106938 doi: 10.1016/j.aml.2020.106938
![]() |
[27] |
L. Yang, X. Pu, Derivation of the burgers equation from the gas dynamics, Commun. Math. Sci., 14 (2016), 671–682. https://doi.org/10.4310/CMS.2016.v14.n3.a4 doi: 10.4310/CMS.2016.v14.n3.a4
![]() |
[28] |
H. Liu, X. Pu, Justification of the NLS approximation for the Euler-Poisson equation, Commun. Math. Phys., 371 (2019), 357–398. https://doi.org/10.1007/s00220-019-03576-4 doi: 10.1007/s00220-019-03576-4
![]() |
[29] |
C. Su, C. Gardner, Korteweg-de Vries equation and generalizations. Ⅲ. Derivation of the Korteweg-de Vries equation and Burgers equation, J. Math. Phys., 10 (1969), 536–539. https://doi.org/10.1063/1.1664873 doi: 10.1063/1.1664873
![]() |
[30] |
L. Song, The Burgers Korteweg-de Vries equation of ionic acoustic waves, Chinese J. space sci., 8 (1988), 57–63. https://doi.org/10.11728/cjss1988.01.053 doi: 10.11728/cjss1988.01.053
![]() |
[31] | J. Lei, P. Yan, A note on conservation law of evolution equations, Math. Appl., 16 (2003), 75–81. |
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