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1.
We analyze global entropy solutions of the 2 × 2 relativistic Euler equations for isentropic fluids in special relativity and establish the uniqueness of Riemann solutions in the class of entropy solutions in L BVloc with arbitrarily large oscillation. The uniqueness result does not require specific reference to any particular method for constructing the entropy solutions. Then the uniqueness of Riemann solutions implies their inviscid time-asymptotic stability under arbitrarily large L1 L BVloc perturbation of the Riemann initial data, provided that the corresponding solutions are in L and have local bounded total variation that allows the linear growth in time. This approach is also extended to deal with the stability of Riemann solutions containing vacuum in the class of entropy solutions in L with arbitrarily large oscillation.Received: October 21, 2003  相似文献   

2.
We analyze global entropy solutions of the 2 × 2 relativistic Euler equations for isentropic fluids in special relativity and establish the uniqueness of Riemann solutions in the class of entropy solutions in L     BVloc with arbitrarily large oscillation. The uniqueness result does not require specific reference to any particular method for constructing the entropy solutions. Then the uniqueness of Riemann solutions implies their inviscid time-asymptotic stability under arbitrarily large L1     L     BVloc perturbation of the Riemann initial data, provided that the corresponding solutions are in L and have local bounded total variation that allows the linear growth in time. This approach is also extended to deal with the stability of Riemann solutions containing vacuum in the class of entropy solutions in L with arbitrarily large oscillation.  相似文献   

3.
1.IntroductionTherehavebeenconsiderableliteratuxeonthedecayofsolutionstothebestialvalueproblemsforsomenonlinearevolutionequations[3,4,6,7,161.Undercertainassumptions,LZdecayandLoodecayofsolutionstotheseproblemswereestablished.Thereadersinterestedcanfindsuchworksinourreferences.OurillterestisfocusedonthedecayofsolutionsoftheinitialvalueproblemsfornonlinearBenjamin--OnthBurgers(BOB)l"'19--21]andSchlodinger-Burgers(SB)equationwhereHisHilberttransform,definedbyWewallttoshowthattheLZandLoon…  相似文献   

4.
Making use of a proper transformation and a generalized ansatz, we consider a new generalized Hamiltonian amplitude equation with nonlinear terms of any order, iux + utt + (|u|p + |u|2p)u + uxt = 0. As a result, many explicit exact solutions, which include kink-shaped soliton solutions, bell-shaped soliton solutions, periodic wave solutions, the combined formal solitary wave solutions and rational solutions, are obtained.Received: April 4, 2002  相似文献   

5.
We study the degenerate parabolic equationut + ∇ · f = ∇ · (Qu) + g, where (x, t) ∈ N × +, the fluxf, the viscosity coefficientQ, and the source termgdepend on (x, t, u) andQis nonnegative definite. Due to the possible degeneracy, weak solutions are considered. In general, these solutions are not uniquely determined by the initial data and, therefore, additional conditions must be imposed in order to guarantee uniqueness. We consider here the subclass of piecewise smooth weak solutions, i.e., continuous solutions which areC2-smooth everywhere apart from a closed nowhere dense collection of smooth manifolds. We show that the solution operator isL1-stable in this subclass and, consequently, that piecewise smooth weak solutions are uniquely determined by the initial data.  相似文献   

6.
The critical exponent of degenerate parabolic systems   总被引:1,自引:0,他引:1  
The Cauchy problemu t=u +v p ,v t =v +u q is studied, wherex R N , 0 <t < and ,,p andq, are positive exponents. It is proved that ifp,q 1 and 1 <pq < 1 + 2 max(p + ,q + )/n then every nontrivial non-negative solution is not global in time; whereaspq > 1 + 2 max(p + , q + )/n then there exist both positive global solutions and non-global solutions. In addition, the decaying in time of solutions tou t,=u inR n × (0, ), an equation which occurs naturally in our study of above systems, is studied and solutions with the fastest decaying in time are constructed.  相似文献   

7.
In this paper, we consider the solutions of the nonlinear Schrödinger equations u/tiu+|u| p u=f andu(x,0)=u 0(x), whereu is defined onR +×R 2. We prove the existence and uniqueness of global weak solutions of the above equations. Lastly, we consider the special case:p=2, and we obtain the strong solutions.  相似文献   

8.
In this article semilinear hyperbolic first order systems in two variables are considered, whose nonlinearity satisfies a global Lipschitz condition. It is shown that these systems admit unique global solutions in the Colombeau algebraG(2). In particular, this provides unique generalized solutions for arbitrary distributions as initial data. The solution inG(2) is shown to be consistent with the locally integrable or the distributional solutions, when they exist.  相似文献   

9.
Summary. In [1], we have constructed a family of finite volume schemes on rectangular meshes for the p-laplacian and we proved error estimates in case the exact solution lies in W2,p. Actually, W2,p is not a natural space for solutions of the p-laplacian in the case p>2. Indeed, for general Lp data it can be shown that the solution only belongs to the Besov space In this paper, we prove Besov kind a priori estimates on the approximate solution for any data in Lp. We then obtain new error estimates for such solutions in the case of uniform meshes  相似文献   

10.
We prove a global existence of solutions for the Landau-Lifshitz equation of the ferromagnetic spin chain from am-dimensional manifoldM into the unit sphereS 2 of 3 and establish some new links between harmonic maps and the solutions of the Landau-Lifshitz equation.  相似文献   

11.
Sufficient conditions are given under which the sequence of the absolute values of all local extremes of y[i], i {0,1,..., n – 2} of solutions of a differential equation with quasiderivatives y [n] = f(t, y [0],..., y [n–1]) is increasing and tends to . The existence of proper, oscillatory and unbounded solutions is proved.  相似文献   

12.
We consider finite time blow-up solutions to the critical nonlinear Schrödinger equation iut=-u-|u|4/Nu with initial condition u0H1. Existence of such solutions is known, but the complete blow-up dynamic is not understood so far. For a specific set of initial data, finite time blow-up with a universal sharp upper bound on the blow-up rate has been proved in [22], [23].We establish in this paper the existence of a universal blow-up profile which attracts blow-up solutions in the vicinity of blow-up time. Such a property relies on classification results of a new type for solutions to critical NLS. In particular, a new characterization of soliton solutions is given, and a refined study of dispersive effects of (NLS) in L2 will remove the possibility of self similar blow-up in energy space H1.  相似文献   

13.
We consider overdetermined nonlinear systems of equationsF(x)=0, whereF: n m ,mn. For this type of systems we define weighted least square distance (WLSD) solutions, which represent an alternative to classical least squares solutions and to other solutions based on residual normas. We introduce a generalization of the classical method of Cimmino for linear systems and we prove local convergence results. We introduce a practical strategy for improving the global convergence properties of the method. Finally, numerical experiments are presented.Work supported by FAPESP (Grant 90/3724/6), FINEP, CNPq and FAEP-UNICAMP.  相似文献   

14.
Making use of a proper transformation and a generalized ansatz, we consider a new generalized Hamiltonian amplitude equation with nonlinear terms of any order, iux  +  utt + (|u|p + |u|2p)u + uxt = 0. As a result, many explicit exact solutions, which include kink-shaped soliton solutions, bell-shaped soliton solutions, periodic wave solutions, the combined formal solitary wave solutions and rational solutions, are obtained.  相似文献   

15.
Let be a C*-algebra, E,F and G be Hilbert -modules, , and . We generalize the Douglas theorem about the operator equation TX=T from Hilbert space to Hilbert C*-module. To the equation TX=T and to the system of two equations TX=T and XS=S, we get the forms of general solutions (in the case that there exists a solution), and give some sufficient and necessary conditions for the existence of solutions, and the existence of hermitian solutions and positive solutions (in the case G=E). In addition, the forms of general hermitian solution and general positive solution (in the case that there exists a solution and G=E) to the equation TX=T are given too.  相似文献   

16.
We prove the nonexistence of solutions for a prescribed mean curvature equation when p?1 and the positive parameter λ is small. The result extends theorems of Narukawa and Suzuki, and Finn, from the case of n=2,p=1 to all n?2,p?1. Moreover, our proof is very simple and the result is not limited to positive (and negative) solutions. We also show that a similar result for positive solutions is still true if |u|p−1u is replaced by the exponential nonlinearity eu−1.  相似文献   

17.
18.
We consider classes of elliptic equations of the form (x,u,u D 2 u)=0 for the solutions of which one establishes local and global a priori estimates for D 2 u=. In particular, one investigates the Monge-Ampere equation, and for its convex solutions one constructs a local and a global estimate for D 2 u and a local estimate for.Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. V. A. Steklova AN SSSR, Vol. 59, pp. 31–59, 1976.  相似文献   

19.
Summary All globally possible solutions of a twisted, homogeneous, elastic ring with circular cross section and no external load are characterized by their symmetry groups. The symmetry group of the untwisted, trivial solution is identified as S t0 = O(2) ×Z 2, and symmetry groups for the nontrivial solutions are found among the subgroups of S t0 .  相似文献   

20.
Summary In this paper we examine the first initial boundary value problem for ut=uxx + (1 – u), > 0, > 0,on (0, 1) × (0, ) from the point of view of dynamical systems. We construct the set of stationary solutions, determine those which are stable, those which are not and show that there are solutions with initial data arbitrarily close to unstable stationary solutions which quench (reach one in finite time). We also examine the related problem ut=uxx, 0 <x < 1,t > 0;u(0,t)=0, (1 – u(1, t)). The set of stationary solutions for this problem, and the dynamical behavior of solutions of the time dependent problem are somewhat different.This research was sponsored by the U.S. Air Force Office of Scientific Research, Air Forse Systems Command Grants 84-0252 and 88-0031. The United States Government is authorized to reproduce and distribute reprints for Governmental purposes not withstanding any copyright notation therein.  相似文献   

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