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1.
This paper deals with the Cauchy problem to the nonlinear pseudo-parabolic system ut-△u-αut=vp,vt-△v-αvt=uqwith p,q 1 and pq1,where the viscous terms of third order are included.We first find the critical Fujita exponent,and then determine the second critical exponent to characterize the critical space-decay rate of initial data in the co-existence region of global and non-global solutions.Moreover,time-decay profiles are obtained for the global solutions.It can be found that,diferent from those for the situations of general semilinear heat systems,we have to use distinctive techniques to treat the influence from the viscous terms of the highest order.To fix the non-global solutions,we exploit the test function method,instead of the general Kaplan method for heat systems.To obtain the global solutions,we apply the Lp-Lq technique to establish some uniform Lmtime-decay estimates.In particular,under a suitable classification for the nonlinear parameters and the initial data,various Lmtime-decay estimates in the procedure enable us to arrive at the time-decay profiles of solutions to the system.It is mentioned that the general scaling method for parabolic problems relies heavily on regularizing efect to establish the compactness of approximating solutions,which cannot be directly realized here due to absence of the smooth efect in the pseudo-parabolic system.  相似文献   

2.
In this paper, we prove the relation v(t)?u(t,x)?w(t), where u(t,x) is the solution of an impulsive parabolic equations under Neumann boundary condition ∂u(t,x)/∂ν=0, and v(t) and w(t) are solutions of two impulsive ordinary equations. We also apply these estimates to investigate the asymptotic behavior of a model in the population dynamics, and it is shown that there exists a unique solution of the model which converges to the periodic solution of an impulsive ordinary equation asymptotically.  相似文献   

3.
Two timing, an ad hoc method for studying periodic evolution equations, can be given a rigorous justification when the problem is in standard form, u = ?f(t, u). First solve dw = ?(I ? M) f(σ, w) for w(σ, v), where M is the mean value operator and v is any initial value. Then w(σ, v) is periodic in σ but does not satisfy the original equation. Now, force a solution u(t), using nonlinear variation of constants, in the form w(σ, v(τ)), where σ = t is the fast time and τ = ?t is the slow time. With the resulting differential equation for v, one reads off from its nonconstant solutions thè approximate transient behavior of u(t) for times of order ??1. On the other hand, the equilibrium points (constant solutions) v0 correspond to steady state (periodic solutions) of the original system. Interesting applications, such as to one-dimensional wave equations with cubic damping, can be given.  相似文献   

4.
We present new decay estimates of solutions for the mixed problem of the equation vtt?vxx+vt=0, which has the weighted initial data [v0,v1]∈(H10(0,∞) ∩L1,γ(0,∞)) × (L2(0,∞)∩L1,γ(0,∞)) (for definition of L1,γ(0,∞), see below) satisfying γ∈[0,1]. Similar decay estimates are also derived to the Cauchy problem in ?N for uttu+ut=0 with the weighted initial data. Finally, these decay estimates can be applied to the one dimensional critical exponent problem for a semilinear damped wave equation on the half line. Copyright © 2004 John Wiley & Sons, Ltd.  相似文献   

5.
We investigate the nonlinear third-order differential equation (uxx ? u)t + u xxx + uux = 0 describing the processes in semiconductors with a strong spatial dispersion. We study the problem of the existence of global solutions and obtain sufficient conditions for the absence of global solutions for some initial boundary value problems corresponding to this equation. We consider examples of solution blowup for initial boundary value and Cauchy problems. We use the Mitidieri-Pokhozhaev nonlinear capacity method.  相似文献   

6.
In this paper, we study certain unique continuation properties for solutions of the semilinear heat equation tu−△u=g(u), with the homogeneous Dirichlet boundary condition, over Ω×(0,T). Ω is a bounded, convex open subset of Rd, with a smooth boundary for the subset. The function g:RR satisfies certain conditions. We establish some observation estimates for (uv), where u and v are two solutions to the above-mentioned equation. The observation is made over ω×{T}, where ω is any non-empty open subset of Ω, and T is a positive number such that both u and v exist on the interval [0,T]. At least two results can be derived from these estimates: (i) if ‖(uv)(⋅,T)L2(ω)=δ, then ‖(uv)(⋅,T)L2(Ω)?Cδα where constants C>0 and α∈(0,1) can be independent of u and v in certain cases; (ii) if two solutions of the above equation hold the same value over ω×{T}, then they coincide over Ω×[0,Tm). Tm indicates the maximum number such that these two solutions exist on [0,Tm).  相似文献   

7.
For the abstract Volterra integro-differential equation utt ? Nu + ∝?∞t K(t ? τ) u(τ) = 0 in Hilbert space, with prescribed past history u(τ) = U(τ), ? ∞ < τ < 0, and associated initial data u(0) = f, ut(0) = g, we establish conditions on K(t), ? ∞ < t < + ∞ which yield various growth estimates for solutions u(t), belonging to a certain uniformly bounded class, as well as lower bounds for the rate of decay of solutions. Our results are interpreted in terms of solutions to a class of initial-boundary value problems in isothermal linear viscoelasticity.  相似文献   

8.
Consider the initial boundary value problem for the linear dissipative wave equation (□+t)u=0 in an exterior domain . Using the so-called cut-off method together with local energy decay and L2 decays in the whole space, we study decay estimates of the solutions. In particular, when N?3, we derive Lp decays with p?1 of the solutions. Next, as an application of the decay estimates for the linear equation, we consider the global solvability problem for the semilinear dissipative wave equations (□+t)u=f(u) with f(u)=|u|α+1,|u|αu in an exterior domain.  相似文献   

9.
We consider a class of continuous non-linear systems defined by the ordinary differential equation x = f(x, t) + g(x, t)u, where u is an unknown input representing noise or disturbances. The object is to estimate states and parameters in these systems by means of a fixed number of discrete observations yi = h(x(ti), ti) + vi, 1 ? i ? m, where the vi represents unknown errors in the measurements yi. No statistical assumptions are made concerning the nature of the unknown input u or the unknown measurement errors vi. A weighted least squares criterion is defined as a measure of the optimal estimate. A result concerning the existence of solutions of the differential equation which minimize the criterion is presented. The necessary conditions for an optimal estimate, a set of Euler-Lagrange equations and multi-point discontinuous non-linear boundary conditions, are given. The multi-point problem is converted to an equivalent continuous two-point boundary value problem of larger dimension in the case in which the observations are assumed to be linear functions of the state. A pair of equivalent quasilinearization algorithms is defined for the two-point system and the multi-point system. Quadratic convergence for these algorithms is proved.  相似文献   

10.
A natural class of appropriate viscosity matrices for strictly hyperbolic systems of conservation laws in one space dimension, u1 + f(u)x = 0, u?Rm, is studied. These matrices are admissible in the sense that small-amplitude shock wave solutions of the hyperbolic system are shown to be limits of smooth traveling wave solutions of the parabolic system ut + f(u)x = v(Dux)x as ifv → 0 if D is in this class. The class is determined by a linearized stability requirement: The Cauchy problem for the equation u1 + f′(u0) ux = vDuxx should be well posed in L2 uniformly in v as v → 0. Previous examples of inadmissible viscosity matrices are accounted for through violation of the stability criterion.  相似文献   

11.
We study the smoothness properties of solutions to the coupled system of equations of Korteweg—de Vries type. We show that the equations dispersive nature leads to a gain in regularity for the solution. In particular, if the initial data (u0, v0 possesses certain regularity and sufficient decay as x → ∞, then the solution (u(t). v(t)) will be smoother than (u0, v0) for 0 < tT where T is the existence time of the solution.  相似文献   

12.
Sufficient conditions are given so that all solutions of the nonlinear differential equation u″ + φ(t, u, u′)u′ + p(t) gf(u) g(u′) = h(t, u, u′) are continuable to the right of an initial t-value t0 ? 0. These conditions are then extended so that all solutions u of the equation in question together with their derivative u′ are bounded for t ? t0 .  相似文献   

13.
In this paper, we study the global existence, L estimates and decay estimates of solutions for the quasilinear parabolic system ut = div (|∇ u|mu) + f(u, v), vt = div (|∇ v|mv) + g(u,v) with zero Dirichlet boundary condition in a bounded domain Ω ⊂ RN. In particular, we find a critical value for the existence and nonexistence of global solutions to the equation ut = div (|∇ u|mu) + λ |u|α - 1 u.  相似文献   

14.
Based on a mixed finite element method, we construct semidiscrete approximations of the solution u and the flux term ?u+?u t of the semilinear Sobolev equations. The existence and uniqueness of the semidiscrete approximations are demonstrated and the error estimates of optimal rate in L 2 normed space are derived. And also we construct the fully discrete approximations of u and ?u+?u t and analyze the convergence of optimal rate in L 2 normed space.  相似文献   

15.
Values of?λ?are determined for which there exist positive solutions of the system of functional differential equations, u″?+?λa(t)f(v t )?=?0,v″?+?λb(t)g(u t )?=?0, for 0?t?u(s)?=?v(s)?=?φ(s), ?r?≤?s?≤?0, and the boundary conditions u(0)?=?v(0)?=?φ(0)?=?u(1)?=?v(1)?=?0. A Guo–Krasnosel'skii fixed point theorem is applied.  相似文献   

16.
Asymptotic properties of solutions of the nonlinear Klein-Gordon equation ?t2u ? Δu + m2u + f(u) = 0 (NLKG) 0 = θ, ?t0 = Ψ, are investigated, which are inherited from the corresponding solutions v of the (linear) Klein-Gordon equation ?t2v ? Δv + m2v = 00 = θ, ?t0 = Ψ, (KG) In particular, the finiteness of time-integrals in Lq over R+ of certain Sobolevnorms in space of the solution is proved to be such a hereditary property. Together with a device by W. A. Strauss and a weak decay result for the (KG) due to R. S. Strichartz, this is used to prove that under suitable restrictions on the nonlinearity, the scattering operator for the (NLKG) is defined on all of L21 × L2 for n = 3.  相似文献   

17.
The paper investigates the structure and properties of the set S of all positive solutions to the singular Dirichlet boundary value problem u″(t) + au′(t)/t ? au(t)/t 2 = f(t, u(t),u′(t)), u(0) = 0, u(T) = 0. Here a ∈ (?,?1) and f satisfies the local Carathéodory conditions on [0,T]×D, where D = [0,∞)×?. It is shown that S c = {uS: u′(T) = ?c} is nonempty and compact for each c ≥ 0 and S = ∪ c≥0 S c . The uniqueness of the problem is discussed. Having a special case of the problem, we introduce an ordering in S showing that the difference of any two solutions in S c ,c≥ 0, keeps its sign on [0,T]. An application to the equation v″(t) + kv′(t)/t = ψ(t)+g(t, v(t)), k ∈ (1,), is given.  相似文献   

18.
《偏微分方程通讯》2013,38(7-8):1385-1408
The purpose of this paper is to study the limit in L 1(Ω), as t → ∞, of solutions of initial-boundary-value problems of the form ut ? Δw = 0 and u ∈ β(w) in a bounded domain Ω with general boundary conditions ?w/?η + γ(w) ? 0. We prove that a solution stabilizes by converging as t → ∞ to a solution of the associated stationary problem. On the other hand, since in general these solutions are not unique, we characterize the true value of the limit and comment the results on the related concrete situations like the Stefan problem and the filtration equation.  相似文献   

19.
Let V?, W?, W and X be Hilbert spaces (0 < ? ? 1) with V? ? W? ? W ? X algebraically and topologically, each space being dense in the one that follows it. For each t? [0, T] let a?(t; u, v), b?(t; u, v) and b(t; u, v) be continuous sesqui-linear forms on V?, W? and W, respectively, which satisfy certain ellipticity conditions. Consider the two equations a?(t; u?, v) + b?(t; u?, v) = 〈f?, v〉 (v?V?) and (u′, v)x + b(t; u, v) = 〈f, v〉 (v?W). Estimates are obtained on the rate of convergence of u? to u, assuming a?(t; u, v) → (u, v)x and b?(t; u, v) → b(t; u, v) in an appropriate sense. These results are then applied to singular perturbation of a class of parabolic boundary value problems.  相似文献   

20.
The study of nonlinear diffusion equations produces a number of peculiar phenomena not present in the standard linear theory. Thus, in the sub-field of very fast diffusion it is known that the Cauchy problem can be ill-posed, either because of non-uniqueness, or because of non-existence of solutions with small data. The equations we consider take the general form ut=(D(u,ux)ux)x or its several-dimension analogue. Fast diffusion means that D→∞ at some values of the arguments, typically as u→0 or ux→0. Here, we describe two different types of non-existence phenomena. Some fast-diffusion equations with very singular D do not allow for solutions with sign changes, while other equations admit only monotone solutions, no oscillations being allowed. The examples we give for both types of anomaly are closely related. The most typical examples are vt=(vx/∣v∣)x and ut=uxx/∣ux∣. For these equations, we investigate what happens to the Cauchy problem when we take incompatible initial data and perform a standard regularization. It is shown that the limit gives rise to an initial layer where the data become admissible (positive or monotone, respectively), followed by a standard evolution for all t>0, once the obstruction has been removed.  相似文献   

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