** Advances in Pure Mathematics
** Vol.3 No.9(2013), Article ID:40882,5 pages DOI:10.4236/apm.2013.39095

A New Application of the Flux Approximation Method on Hyperbolic Conservation Systems

^{1}Department of Mathematics, Hangzhou Normal University, Hangzhou, China

^{2}Departamento de Matemáticas, Universidad Nacional de Colombia, Bogotá, Colombia

Email: ^{*}deyinzheng@hznu.edu.cn

Copyright © 2013 Yunguang Lu et al. 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. In accordance of the Creative Commons Attribution License all Copyrights © 2013 are reserved for SCIRP and the owner of the intellectual property Yunguang Lu et al. All Copyright © 2013 are guarded by law and by SCIRP as a guardian.

Received November 14, 2013; revised December 8, 2013; accepted December 15, 2013

**Keywords:** Flux Approximation; Viscosity Approximation; Hyperbolic Conservation Laws; Weak Solutions; Compensated Compactness Method

ABSTRACT

In this paper, we first summarize several applications of the flux approximation method on hyperbolic conservation systems. Then, we introduce two hyperbolic conservation systems (2.1) and (2.2) of Temple’s type, and prove that the global weak solutions of each system could be obtained by the limit of the linear combination of two systems.

1. Introduction

It is well known that no classical solution exists for the following initial value problem

(1.1)

with bounded measurable initial data

(1.2)

where is the unknown vector function standing for the density of physical quantities and is a given vector function denoting the conservative term. These equations are commonly called conservation laws.

Since, in general, the discontinuity or the shock waves will appear in the solution to the Cauchy problem (1.1)- (1.2), there are two standard methods to obtain a weak solution or a generalized solution for given hyperbolic conservation laws. One is to construct a sequence of smooth functions to approximate. For example, to add a small parabolic perturbation term to the right-hand side of (1.1):

(1.3)

where is a constant. For each fixed, we have a classical solution of (1.3)-(1.2), then we try to prove that the limit of as goes to zero is the solution of (1.1)-(1.2), where the compactness could be obtained by the compensated compactness arguments [1,2] when the functions have only the uniform boundedness in a suitable Banach space or the technique given in [3] when the functions are of total bounded variation estimates; another is the finite difference method [4]. We construct a sequence of simple functions by choosing a suitable difference scheme which is based on the given hyperbolic conservation laws and then prove the compactness of the sequence of functions. Normally, in the second method, we know that the sequence of simple functions is of total bounded variation estimates.

However, the third front tracking method [5], here we just call it the flux approximation method, is also used in many different cases.

In [6], Dafermos first introduced this method to the scalar conservation law

(1.4)

where is a scalar function, and is a locally Lipschitz continuous function. He constructed a sequence of piecewise linear functions and a sequence of step functions to approximate and the initial date respectively. Let the solutions of the following Cauchy problem be:

(1.5)

with the initial data

(1.6)

For each fixed, since the simplicity of the flux function and the initial date, the sequence of solutions can be easily obtained first. Then by using the standard compactness argument by Oleinik, the convergence of can be proved as goes to zero.

Later, the above idea was used to study the existence of Riemann solutions for some special systems of two equations. For example, in [7], the author first studied the Riemann solution for the Cauchy problem of the following system

(1.7)

with initial data

(1.8)

The more details about the Front Tracking method for systems of hyperbolic conservation laws can be found in the books [5,8] and the references cited therein.

In [9], Keyfitz introduced a different way to approximate the nonlinear flux function. Consider the Cauchy problem

(1.9)

with the Riemann initial data, where since the system is hyperbolic or as required in

[9]. For each fixed, System (1.9) is strictly hyperbolic and Riemann solution could be easily obtained. Then a Riemann solution of system (1.7) follows since it is the limit of as goes to zero.

The method of flux approximation was applied by the first author of this paper to study the existence of weak solutions [10,11], the existence of global Lipschitz solutions [12], compactness for weak entropy-entropy flux pairs of the isentropic gas dynamics [11], estimate for isentropic gas dynamics with a superline source [13], the global solutions of Aw-Rascle traffic flow model [14] (or the nonsymmetric systems of Keyfitz-Kranzer type) with negative adiabatic exponent and so on, which we shall introduce below. A new application of this method related to the LeRoux system is introduced in Theorem 1, Section 2.

2. A New Application of Flux Approximation Method

In this section, we introduce a new application of the flux approximation method. We found two hyperbolic conservation systems of Temple’s type [15], and the global weak solution of each system could be obtained by the limit of the linear combination of two systems.

Consider the hyperbolic systems

(2.1)

and

(2.2)

By simple calculations, two eigenvalues of system (2.1) are

(2.3)

where, with corresponding right eigenvectors

(2.4)

and

(2.5)

The Riemann invariants of (2.1) are

(2.6)

Thus, the curves are straight lines on the -plane.

Similarly, two eigenvalues of system (2.2) are

(2.7)

with the corresponding right eigenvectors (2.4) and

(2.8)

The Riemann invariants of (2.2) are also given by (2.6)

Therefore if we consider the bounded solution in the region:, it follows from (2.5) (or (2.8)) that both characteristic fields of system (2.1) (or system (2.2)) are genuinely nonlinear in the sense of Lax [16].

Now we prove that both systems (2.1) and (2.2) have the same entropies.

Let. Then for smooth solutions, (2.2) is equivalent to the following system:

(2.9)

Considering the entropy-entropy flux pair of system (2.2) as functions of variables, we have

(2.10)

Eliminating the from (2.10), we have

(2.11)

Similarly, for smooth solutions, (2.1) is equivalent to the following system:

(2.12)

For the entropy-entropy flux pair of system (2.1), we have

(2.13)

Eliminating the from (2.13), we have also the same entropy Equation (2.11).

Using the compensated compactness arguments, we may easily obtain the global existence of weak solutions for the Cauchy problem of system (2.2) in the upper -plane or system (2.1) in the region for a suitable constant, which could be guaranteed since the curves are straight lines, where are four suitable constants. The details could be found in Chapter 7 of [17] or the original paper by Diperna [18].

Now we consider the linear combination of systems (2.1) and (2.2):

(2.14)

where are two positive flux approximation perturbations.

The eigenvalues of system (2.14) are solutions of the following characteristic equation:

(2.15)

Two roots of Equation (2.15) are

(2.16)

with the corresponding right eigenvectors (2.4) and the Riemann invariants (2.6). Moreover,

(2.17)

Therefore both characteristic fields of system (2.14) are genuinely nonlinear in the region:.

Now we consider the Cauchy problem of system (2.14) with initial data

(2.18)

and have the main results in the following theorem

**Theorem 1.** Suppose the initial data be bounded measurable and for a suitable constant. Then for any fixed, the global weak solution of the Cauchy problem (2.14) and (2.18) exists. Moreover, for fixed (or), there exists a subsequence (or) of, which piontwisely converges, as (or) goes to zero, to the solution of the Cauchy problem of system (2.1) (or (2.2)) with the initial data (2.18).

**The proof of Theorem 1:** The proof of Theorem 1 can be obtained by the standard vanishing artificial viscosity method coupled with the compensated compactness argument and the famous framework of DiPerna [18] for strictly hyperbolic, genuinely nonlinear systems of two equations. We add the viscosity terms to the right hand side of (2.14) and consider the following parabolic system

(2.19)

with the initial data (2.18). According to the calculations given in (2.3) and (2.7), we know that the two eigenvalues of system (2.14) are

(2.20)

with the corresponding right eigenvectors (2.4) and the Riemann invariants (2.6).

For any constant, the curves or is a straight line on the -plane, then we may choose suitable constants such that forms a bounded invariant region. Moreover, in this region, for a suitable constant. Since system (2.14) is strictly hyperbolic and genuinely nonlinear, and the viscosity solutions of system (2.19) are uniformly bounded, then the famous compactness framework of DiPerna [18] gives us the convergence of

(2.21)

where the limit is a weak solution of system (2.14) or satisfies (2.14) in the sense of distributions. For fixed (or), and for the generalized functions, we may rewrite system (2.14) as

(2.22)

Since the left hand side of (2.22) or system (2.1) is also strictly hyperbolic and genuinely nonlinear, and the functions are uniformly bounded, independent of, so the DiPerna’s result [18] reduces the following convergence

(2.23)

where the limit is a weak solution of system (2.1) or satisfies (2.1) in the sense of distributions, which ends the proof of Theorem 1.

3. Acknowledgements

This work was partially supported by the Natural Science Foundation of Zhejiang Province of China (Grant No. LY12A01030 and Grant No. LZ13A010002) and the National Natural Science Foundation of China (Grant No. 11271105).

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NOTES

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