Discrete Dynamics in Nature and Society
Volume 2020 (2020), Article ID 2757398, 8 pages
https://doi.org/10.1155/2020/2757398

Research Article

The Singularity Formation on the Coupled Burgers–Constantin–Lax–Majda System with the Nonlocal Term

Linrui Li¹ and Shu Wang²

¹Basic Courses Department, Institute of Disaster Prevention, Yanjiao, Sanhe, Hebei 065201, China
²School of Mathematics and Information Sciences, Guangzhou University, Guangzhou 510006, Guangdong, China

Correspondence should be addressed to Linrui Li; linrui020213@163.com

Received 9 April 2020; Accepted 12 June 2020; Published 17 July 2020

Academic Editor: Ciprian G. Gal

Copyright © 2020 Linrui Li and Shu Wang. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

In this paper, we study the finite-time singularity formation on the coupled Burgers–Constantin–Lax–Majda system with the nonlocal term, which is one nonlinear nonlocal system of combining Burgers equations with Constantin–Lax–Majda equations. We discuss whether the finite-time blow-up singularity mechanism of the system depends upon the domination between the CLM type’s vortex-stretching term and the Burgers type’s convection term in some sense. We give two kinds of different finite-time blow-up results and prove the local smooth solution of the nonlocal system blows up in finite time for two classes of large initial data.

1. Introduction

We study the formation of singularities for the following coupled Burgers–Constantin–Lax–Majda system with the nonlocal term:

where are the given constants and is the Hilbert transform operator defined by

or defined by the Fourier transform by

In the following, we will use the fractional operator with , which is defined by and can be given by

where .

System (1) possesses the nonlocal nonlinear term and the local nonlinear term . If , it recovers back to the famous Constantin–Lax–Majda (CLM) system:

which is one nonlocal nonlinear system proposed by Constantin et al. in [1] as a simplified 1D system for the 3D vorticity model on the incompressible Euler equation. It should be pointed out that the question on the finite-time singularity formation of the CLM model is considered to be closely related to the most outstanding mathematical open problems on the three-dimensional incompressible Euler equation. In (5), the nonlocal nonlinear term is one kind of one-dimensional approximation of the vortex-stretching term in the three-dimensional incompressible Euler equation. If and , system (1) recovers back to the classical Burgers system in the conservation law field, where its general form with the viscosity is given by (see [2, 3])

It is known that the solutions to two systems, both the CLM system and the Burgers system, have the characteristic of finite-time blow-up singularity formation for the smooth solutions with the smooth initial data. When and , system (1) possesses both the CLM type’s nonlocal term and the (local) generalized Burgers type’s convection term .

We also recall some related problems on the finite-time blow-up singularity regimes about some models with the Hilbert transform and the generalized Burgers equations. Gregorio proposed the following system

as another simplified model of the 3D vorticity version of incompressible inviscid Euler flow in [4, 5] and obtained some numeric results which implied that the convection term seems to prevent the appearance of finite-time blow-up singularity. Recently, Lei et al. [6] proved that there exist global smooth solutions to system (7) for a class of large nonnegative initial data. Okamoto et al. [7] suggested the generalized CLM system

with as a parameter. Catro and Córdoba [8] proved the finite-time blow-up singularity for the solution to system (8) when from a class of smooth initial data. Córdoba et al. [9, 10] studied the system and obtained the finite-time blow-up results for the smooth initial data. Sakajo [11] studied the CLM equation with the generalized viscosity term , where they gave the explicit solution and obtained the finite-time blow-up result for the smooth initial data. Hou et al. [12] investigated the singularity formation of a nonlinear nonlocal system,

and proved the finite-time blow-up result for a class of large initial data and the global existence result for another initial data for the Cauchy or periodic problem to system (9). Recently, Choi et al. [13] studied the finite-time blowup of a one-dimensional model from the three-dimensional axisymmetric Euler equations and obtained the finite-time blow-up result for the smooth initial data.

Kiselev et al. [14] studied the blow-up and regularity problem for the fractal Burgers equation . Castro et al. [15] studied the singularity formation of a surface wave model (where ) and obtained the finite-time singularity result when . Hur [16] discussed the generalized surface wave model (where or and ) and proved the finite-time singularity result. Hunter and Ifrim [17] discussed the lifespan of the smooth solutions of a Burgers–Hilbert equation over cubically nonlinear time scales on .

Meanwhile, we remark that there are a lot of research studies carried out on nonlocal different equations. Coclite et al. [18] obtained the formation of singularities in finite time in nonlocal Burgers equations with the time-fractional derivative and employed Burgers equations to model a problem arising in the job market. Wang and Zhang [19] established the nonexistence of positive solutions to nonlocal Lane–Emden equations and obtained the “Fujita index” for nonlocal reaction-diffusion equations, which is new in the blow-up theory. In this paper, motivated by the above results on the CLM system and the generalized Burgers system with the nonlocal operator, we study the finite-time blow-up singularity mechanism of system (1). We would like to discuss whether the finite-time blow-up singularity mechanism of the system depends upon the domination between the CLM type’s vortex stretching and the Burgers type’s convection in some sense. We will give two kinds of different finite-time blow-up singularity regimes for two classes of initial data. One mechanism seems to be caused by the domination of the vortex-stretching term of the system, see (17)–(19), which is of CLM’s finite-time blow-up mechanism type, but another seems to be caused by the domination of the convection term of the system, see (42) and (43), which is of Burgers’ finite-time blow-up mechanism type. That is to say that the coupled Burgers–Constantin–Lax–Majda system possesses two kinds of finite-time blow-up singularity regimes of both the Constantin–Lax–Majda system and the Burgers system.

The rest of this paper is as follows. The main results of this paper are given in Section 2, and Section 3 is devoted to the proofs of the main results of Section 2.

2. Main Results

In this section, we give the main results of this paper.

Theorem 1. Let and . Also, let . Assume that there exists such that

Then, there is finite time such that the solution to system (1) blows up in finite time.

Theorem 2. Let and . Also, let and be given and be the solution to the algebra equation

where which are given by

Assume that there exists such that

Then, there is finite time such that the solution to system (1) blows up in finite time.

Remark 1. For the coupled Burgers–CLM equation, it is obvious that the system is -conservative on the norm of the nonnegative solution by using the property of Hilbert transform .

Remark 2. Assumption (10) on initial data in Theorem 1 to guarantee the finite-time blow-up mechanism for system (1) is completely the same as the one for CLM system (5). However, assumption (13) on initial data in Theorem 2 is completely different from assumption (10), which yields to another finite-time blow-up mechanism for system (1). That is to say that there are two kinds of the finite-time blow-up regimes. One blow-up regime, given by Theorem 1, is caused by the nonlocal nonlinear term related to the vortex-stretching term, while another regime given by Theorem 2 comes from Burgers’ type convection term. This reflects that the modes of the finite-time blow-up regimes may depend upon the domination between the CLM type’s vortex-stretching term and the Burgers’ type convection term in some sense.

Remark 3. The assumption condition in (13) can be replaced by , and Theorem 2 still holds.

3. The Proof of the Main Results

To finish the proof of the main results, we, firstly, recall some basic properties of the Hilbert transform (see [1]).

Lemma 1.

Now, we give the proof of Theorem 1 by using Lemma 1.

Proof of Theorem 1. For the local existence and uniqueness of the smooth solution in the class of to system (1), it can be obtained by the iteration technique and by using the existence and uniqueness theory of the linearized hyperbolic equation. This is standard, and we omit it here. Also, it is obvious that the solution only if .
Taking the Hilbert operator on (1), we get, with the help of Lemma 1, that

Taking in (16) and using assumption (10) on the initial data, we get

Combining (17) and (18), we have

According to the theory on the nonlinear ODE and by using in assumption (10) on the initial data, we can get from (19) that blows up in finite time.
This completes the proof of Theorem 1.
Next, to prove Theorem 2, we give a local nonnegative lower bound estimate on the nonlocal term , which plays the key role on proving the main result of Theorem 2 of this paper. In fact, it is an extension version of Lemma 2 in the paper [15], where the case that is obtained. For completeness, we give its proof here.

Lemma 2. Let with , and let and be given. Then, for any fixed point satisfying , we have

where is given by (12) in Theorem 2.

Proof. Let be the set

where will be given in the following. And let be the subsets of such that

In the following, will be chosen to be such that and . Obviously, .
On the one hand, using the fact

we have

By Young’s inequality with , we get

which yields to

Combining (24) with (26), we have

Here, we need , i.e., .
On the other hand, we have

which yields to

Since and , we have, by combining (27) and (29), that

Now, we choose for fixed satisfying . Thus, we get from (30) that

which gives (20). This completes the proof of Lemma 2.

Remark 4. Under the assumption of Lemma 2, inequality (20) holds still for the point such that because .

Proof of Theorem 2. First, it is easy to prove that there is a unique smooth solution of system (1) for some time .
Now, we want to prove the solution will blow up in finite time for some classes of large initial data in the sense of our assumption. We end this by a contradiction argument. Assume that there exists the global solution for all time .
Firstly, for the solution of system (1), there exists one conservation law, see Remark 1:

Then, we define the particle trajectories by the equation

It follows from systems (1) and (33) that

which yields to

Thus, it follows from (35) that for any if for some fixed , and for any finite if for some fixed .
For any fixed satisfying (especially, this is true for in Theorem 2), it follows from (34) that

and, hence, by using (16), (32), and (20) in Lemma 2, we have

Here, we have used , , and .
By Young’s inequality, we have

where is given by (13) in Theorem 2.
Putting (38) into (37), we have

Now, setting

then, by (39) and (40), we have

By the existence-uniqueness and extension theory of ordinary differential equations, we know that the solution of system (40) is nondecreasing with respect to the time and for fixed and satisfies and as if for some fixed , where is the solution to algebra equation (11). In fact, here, by using (36).
Taking especially, where is given in Theorem 2, by the assumption on Theorem 2, we have that . Hence, it is obvious that there exists time such that is nondecreasing for , and satisfies , , and .
Also, taking in (39), we have, for all , that

Integrating (42) with respect to from to , we have

which, by integrating (43) with respect to from to , gives

Since , we have

Combining (44) with (45), we have

Let

Then, by (46), we have

Multiplying the first equation of (47) by and then integrating the resulting equation, we have

Let we have

That is to say

and, hence,

which gives

Taking to be

when in (53), we have

which implies that the maximal existence time to the solution of (1) cannot be extended more than . This is a contradiction with the assumption that the solution is global in time. The proof of Theorem 2 is complete.

Data Availability

No data were used to support this study.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Acknowledgments

The research of L. R. Li was supported by the Scientific Research Plan Projects for Higher Schools in Hebei Province (Grant no. QN2019308) and Special Fund of Fundamental Scientific Research Business Expense for Higher School of Central Government (Projects for young teachers, Grant no. ZY20180212). The research of S. Wang was partially supported by the National Science Foundation of China (Grant nos. 11531010, 11831003, and 11771031) and Qinghai Science Foundation of China. The research was also funded by the China Scholarship Council (no. 201902025001).

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