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1.
Let Ω be an open bounded set in ℝN, N≥3, with connected Lipschitz boundary ∂Ω and let a(x,ξ) be an operator of Leray–Lions type (a(⋅,∇u) is of the same type as the operator |∇u|p−2u, 1<p<N). If τ is the trace operator on ∂Ω, [φ] the jump across ∂Ω of a function φ defined on both sides of ∂Ω, the normal derivative ∂/∂νa related to the operator a is defined in some sense as 〈a(⋅,∇u),ν〉, the inner product in ℝN, of the trace of a(⋅,∇u) on ∂Ω with the outward normal vector field ν on ∂Ω. If β and γ are two nondecreasing continuous real functions everywhere defined in ℝ, with β(0)=γ(0)=0, fL1(ℝN), gL1(∂Ω), we prove the existence and the uniqueness of an entropy solution u for the following problem,
in the sense that, if Tk(r)=max {−k,min (r,k)}, k>0, r∈ℝ, ∇u is the gradient by means of truncation (∇u=DTku on the set {|u|<k}) and , u measurable; DTk(u)∈Lp(ℝN), k>0}, then and u satisfies,
for every k>0 and every . Mathematics Subject Classifications (2000)  35J65, 35J70, 47J05.  相似文献   

2.
LetM be a compact riemannian manifold,h an odd function such thath(r)/r is non-decreasing with limit 0 at 0. Letf(r)=h(r)-γr and assume there exist non-negative constantsA andB and a realp>1 such thatf(r)>Ar P-B. We prove that any non-negative solutionu ofu ttgu=f(u) onM x ℝ+ satisfying Dirichlet or Neumann boundary conditions on ϖM converges to a (stationary) solution of Δ g Φ=f(Φ) onM with exponential decay of ‖u-Φ‖C 2(M). For solutions with non-constant sign, we prove an homogenisation result for sufficiently small λ; further, we show that for every λ the map (u(0,·),u t(0,·))→(u(t,·), u t(t,·)) defines a dynamical system onW 1/2(M)⊂C(M)×L 2(M) which possesses a compact maximal attractor.   相似文献   

3.
In this work we prove that the initial value problem of the Benney-Lin equation ut + uxxx + β(uxx + u xxxx) + ηuxxxxx + uux = 0 (x ∈ R, t ≥0 0), where β 〉 0 and η∈R, is locally well-posed in Sobolev spaces HS(R) for s ≥ -7/5. The method we use to prove this result is the bilinear estimate method initiated by Bourgain.  相似文献   

4.
We study the continuous as well as the discontinuous solutions of Hamilton-Jacobi equationu t +H(u,Du) =g in ℝ n x ℝ+ withu(x, 0) =u 0(x). The HamiltonianH(s,p) is assumed to be convex and positively homogeneous of degree one inp for eachs in ℝ. IfH is non increasing ins, in general, this problem need not admit a continuous viscosity solution. Even in this case we obtain a formula for discontinuous viscosity solutions.  相似文献   

5.
Summary We consider a model of random walk on ℤν, ν≥2, in a dynamical random environment described by a field ξ={ξ t (x): (t,x)∈ℤν+1}. The random walk transition probabilities are taken as P(X t +1= y|X t = x t =η) =P 0( yx)+ c(yx;η(x)). We assume that the variables {ξ t (x):(t,x) ∈ℤν+1} are i.i.d., that both P 0(u) and c(u;s) are finite range in u, and that the random term c(u;·) is small and with zero average. We prove that the C.L.T. holds almost-surely, with the same parameters as for P 0, for all ν≥2. For ν≥3 there is a finite random (i.e., dependent on ξ) correction to the average of X t , and there is a corresponding random correction of order to the C.L.T.. For ν≥5 there is a finite random correction to the covariance matrix of X t and a corresponding correction of order to the C.L.T.. Proofs are based on some new L p estimates for a class of functionals of the field. Received: 4 January 1996/In revised form: 26 May 1997  相似文献   

6.
We study the Cauchy problem for the nonlinear dissipative equations (0.1) uo∂u-αδu + Β|u|2/n u = 0,x ∃ Rn,t } 0,u(0,x) = u0(x),x ∃ Rn, where α,Β ∃ C, ℜα 0. We are interested in the dissipative case ℜα 0, and ℜδ(α,Β) 0, θ = |∫ u0(x)dx| ⊋ 0, where δ(α, Β) = ##|α|n-1nn/2 / ((n + 1)|α|2 + α2 n/2. Furthermore, we assume that the initial data u0 ∃ Lp are such that (1 + |x|)αu0 ∃ L1, with sufficiently small norm ∃ = (1 + |x|)α u0 1 + u0 p, wherep 1, α ∃ (0,1). Then there exists a unique solution of the Cauchy problem (0.1)u(t, x) ∃ C ((0, ∞); L) ∩ C ([0, ∞); L1 ∩ Lp) satisfying the time decay estimates for allt0 u(t)|| Cɛt-n/2(1 + η log 〈t〉)-n/2, if hg = θ2/n 2π ℜδ(α, Β) 0; u(t)|| Cɛt-n/2(1 + Μ log 〈t〉)-n/4, if η = 0 and Μ = θ4/n 4π)2 (ℑδ(α, Β))2 ℜ((1 + 1/n) υ1-1 υ2) 0; and u(t)|| Cɛt-n/2(1 + κ log 〈t〉)-n/6, if η = 0, Μ = 0, κ 0, where υl,l = 1,2 are defined in (1.2), κ is a positive constant defined in (2.31).  相似文献   

7.
In this paper we consider abstract equations of the typeK ν ν +ν =w 0, in a closed convex subset of a separable Hilbert spaceH. For eachv in the closed convex subset,K v :HH is a bounded linear map. As an application of our abstract result we obtain an existence result for nonlinear integral equations of the typeν(s)+ν(s) 0 1 k(s,t)ν(t)dt =W 0(s) in the spaceL 2 [0,1].  相似文献   

8.
We present existence principles for the nonlocal boundary-value problem (φ(u(p−1)))′=g(t,u,...,u(p−1), αk(u)=0, 1≤k≤p−1, where p ≥ 2, π: ℝ → ℝ is an increasing and odd homeomorphism, g is a Carathéodory function that is either regular or has singularities in its space variables, and α k: C p−1[0, T] → ℝ is a continuous functional. An application of the existence principles to singular Sturm-Liouville problems (−1)n(φ(u(2n−)))′=f(t,u,...,u(2n−1)), u(2k)(0)=0, αku(2k)(T)+bku(2k=1)(T)=0, 0≤k≤n−1, is given. Published in Ukrains’kyi Matematychnyi Zhurnal, Vol. 60, No. 2, pp. 240–259, February, 2008.  相似文献   

9.
In this paper we study the boundary limit properties of harmonic functions on ℝ+×K, the solutions u(t,x) to the Poisson equation
\frac?2 u?t2 + Du = 0,\frac{\partial^2 u}{\partial t^2} + \Delta u = 0,  相似文献   

10.
This paper is concerned with solutions of the Hamiltonian system: [(u)\dot]=JHu(t,u)\dot{u}=\mathcal{J}H_{u}(t,u) , where H(t,u)=\frac12u·Lu+W(t,u)H(t,u)=\frac{1}{2}u\cdot Lu+W(t,u) with L being a 2N×2N symmetric matrix and WC 1(ℝ×ℝ2N ,ℝ) being super quadratic at infinity in u∈ℝ2N . We use variational methods to study this problem. By virtue of some auxiliary system related to the “limit equation” of the Hamiltonian system, we constructed linking levels of the variational functional Φ such that the minimax value E l based on the linking structure of Φ satisfies 0 < El < El00El0E_{l_{0}} is the least action of the “limit equation”. Thus we can show the (PS) c -condition holds true for all c < El0c相似文献   

11.
We study a periodic boundary-value problem for the quasilinear equation u tt u xx =F[u, u t , u x ], u(x, 0)=u(x, π)=0, u(x + ω, t) = u(x, t), x ∈ ℝ t ∈ [0, π], and establish conditions that guarantee the validity of a theorem on unique solvability. Translated from Ukrainskii Matematicheskii Zhurnal, Vol. 50, No. 9, pp. 1293–1296, September, 1998.  相似文献   

12.
In three spaces, we find exact classical solutions of the boundary-value periodic problem utt - a2uxx = g(x, t) u(0, t) = u(π, t) = 0, u(x, t + T) = u(x, t), x ∈ ℝ, t ∈ ℝ. We study the periodic boundary-value problem for a quasilinear equation whose left-hand side is the d’Alembert operator and whose right-hand side is a nonlinear operator. Translated from Ukrainskii Matematicheskii Zhurnal, Vol. 50, No. 12, pp. 1680–1685, December, 1998.  相似文献   

13.
The celebrated result by Baras and Goldstein (1984) established that the heat equation with the inverse square potential in the unit ball B 1 ⊂ ℝ N , N ≥ 3, u t = Δ u + in B 1 × (0,T), u|∂B 1 = 0, in the supercritical range c > c Hardy = does not have a solution for any nontrivial L 1 initial data u 0(x) ≥ 0 in B 1 (or for a positive measure u 0). More precisely, it was proved that a regular approximation of a possible solution by a sequence {u n (x,t)} of classical solutions corresponding to truncated bounded potentials given by V(x) = ↦ V n (x) = min{, n} (n ≥ 1) diverges; i.e., as n → ∞, u n (x,t) → + ∞ in B 1 × (0, T). Similar features of “nonexistence via approximation” for semilinear heat PDEs were inherent in related results by Brezis-Friedman (1983) and Baras-Cohen (1987). The main goal of this paper is to justify that this nonexistence result has wider nature and remains true without the positivity assumption on data u 0(x) that are assumed to be regular and positive at x = 0. Moreover, nonexistence as the impossibility of regular approximations of solutions is true for a wide class of singular nonlinear parabolic problems as well as for higher order PDEs including, e.g., u t = , and , N > 4. Dedicated to Professor S.I. Pohozaev on the occasion of his 70th birthday  相似文献   

14.
Let u be harmonic in a simply connected domainG ⊂ ℝ2 and letK be a compact subset of G. In this note, it is proved there exists an “elliptic continuation” of u, namely there exist a smooth functionu 1 and a second order uniformly elliptic operatorL with smooth coefficients in ℝ2, satisfying:u 1=u inK, Lu 1=0 in ℝ2. A similar continuation theorem, with u itself a solution to an elliptic second order equation inG, is also proved.  相似文献   

15.
Let a1,a2, . . . ,am ∈ ℝ2, 2≤fC([0,∞)), giC([0,∞)) be such that 0≤gi(t)≤2 on [0,∞) ∀i=1, . . . ,m. For any p>1, we prove the existence and uniqueness of solutions of the equation ut=Δ(logu), u>0, in satisfying and logu(x,t)/log|x|→−f(t) as |x|→∞, logu(x,t)/log|xai|→−gi(t) as |xai|→0, uniformly on every compact subset of (0,T) for any i=1, . . . ,m under a mild assumption on u0 where We also obtain similar existence and uniqueness of solutions of the above equation in bounded smooth convex domains of ℝ2 with prescribed singularities at a finite number of points in the domain.  相似文献   

16.
 We prove that the solution u of the equation u t =Δlog u, u>0, in (Ω\{x 0})×(0,T), Ω⊂ℝ2, has removable singularities at {x 0}×(0,T) if and only if for any 0<α<1, 0<a<b<T, there exist constants ρ0, C 1, C 2>0, such that C 1 |xx 0|αu(x,t)≤C 2|xx 0|−α holds for all 0<|xx 0|≤ρ0 and atb. As a consequence we obtain a sufficient condition for removable singularities at {∞}×(0,T) for solutions of the above equation in ℝ2×(0,T) and we prove the existence of infinitely many finite mass solutions for the equation in ℝ2×(0,T) when 0≤u 0L 1 (ℝ2) is radially symmetric and u 0L loc 1(ℝ2). Received: 16 December 2001 / Revised version: 20 May 2002 / Published online: 10 February 2003 Mathematics Subject Classification (1991): 35B40, 35B25, 35K55, 35K65  相似文献   

17.
This paper deals with conditions for the existence of solutions of the equations
considered in the whole space ℝn, n ≥ 2. The functions A i (x, u, ξ), i = 1,…, n, A 0(x, u), and f(x) can arbitrarily grow as |x| → ∞. These functions satisfy generalized conditions of the monotone operator theory in the arguments u ∈ ℝ and ξ ∈ ℝn. We prove the existence theorem for a solution uW loc 1,p (ℝn) under the condition p > n. __________ Translated from Fundamentalnaya i Prikladnaya Matematika, Vol. 12, No. 4, pp. 133–147, 2006.  相似文献   

18.
In this paper we establish some oscillation or nonoscillation criteria for the second order half-linear differential equation
where (i) r,cC([t 0, ∞), ℝ := (− ∞, ∞)) and r(t) > 0 on [t 0, ∞) for some t 0 ⩾ 0; (ii) Φ(u) = |u|p−2 u for some fixed number p > 1. We also generalize some results of Hille-Wintner, Leighton and Willet.  相似文献   

19.
One considers a semilinear parabolic equation u t = Lua(x)f(u) or an elliptic equation u tt + Lua(x)f(u) = 0 in a semi-infinite cylinder Ω × ℝ+ with the nonlinear boundary condition , where L is a uniformly elliptic divergent operator in a bounded domain Ω ∈ ℝn; a(x) and b(x) are nonnegative measurable functions in Ω. One studies the asymptotic behavior of solutions of such boundary-value problems for t → ∞. __________ Translated from Trudy Seminara imeni I. G. Petrovskogo, No. 26, pp. 368–389, 2007.  相似文献   

20.
This paper deals with the blow-up properties of solutions to a system of heat equations u tu, v tv in B R×(0, T) with the Neumann boundary conditions εu/εη=e v, εv/εη=e u on S R×[0, T). The exact blow-up rates are established. It is also proved that the blow-up will occur only on the boundary. This work is supported by the National Natural Science Foundation of China  相似文献   

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