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1.
本文处理带非线性边界条件 u n=uα, v n=vβ ,(x ,t) ∈ Ω× (0 ,T)的抛物方程组ut =vpΔu ,vt=uqΔv ,(x ,t) ∈Ω× (0 ,T) ,其中Ω RN 为一个有界区域 ,p ,q>0和α ,β≥ 0为常数 .研究了上述问题正解的整体存在性和爆破 ,建立了整体存在和爆破的新标准 .证明了当max{p+β,q+α}≤ 1时正解 (u ,v)整体存在 ,当min{p+β ,q+α}>1且max{α ,β}<1时正解 (u ,v)在有限时刻爆破  相似文献   

2.
讨论了一类具有奇异系数的p-Laplace问题-Δpu-μ|u|u|x|p=u|x|tu+λuq-2u,x∈Ω,u=0,x∈Ω无穷多解的存在性,其中N≥3,Ω是RN中一有界光滑区域,0∈Ω,Δpu=-div(|▽u|p-2▽u),0≤μ<μ=(N-p)ppp,10,1相似文献   

3.
本文研究下述具有变指数反应项的多孔介质方程解的爆破和整体存在性问题,u_t=?u~m+u~(p(x)),(x,t)∈?×(0,T),其中?为有界域或全空间R~N,p(x)为定义在?上满足条件0p_=infp(x)≤p(x)≤p+=supp(x)∞的连续函数.这个方程由于变指数p(x)与定义域?的空间结构之间的相互作用表现出丰富而有趣的动力学特性.粗略地讲,对于全空间R~N上的初值问题,如果p(x)≤1,则方程的解可能不具有唯一性,此时所有非平凡解均整体存在;如果p+m,此时一定存在爆破解.进一步,当1p(x)≤m+2/N时,所有非平凡解均爆破;当p(x)m+2/N时,存在非平凡整体解.当p_m+2/N时,本文构造的例子表明,对于某些p(x)所有非平凡解均爆破;而对于另外一些p(x),则可能存在整体非平凡解.在有界域上解的性质与全空间又有所不同.此时有p(x)和m及区域性质三个因素相互作用,而仅有一个临界指标p=m表征解的爆破行为.若p+m,则此时如同全空间情形存在爆破解;若p+m,则方程所有解均整体存在;又若p(x)m或者区域足够小,则方程存在整体解.最有意思的是,对于某些满足条件p_mp+的p(x),作者发现了对于这类方程特有的有界域上的Fujita现象.  相似文献   

4.
该文研究光滑有界区域Ω( RN (N≥ 1) 上具有齐次Dirichlet边界条件的拟线性退化抛物型方程组 ut-div(|▽u|p-2 ▽u) =avα, vt-div(|▽v|q-2 ▽v) =buβ 的非负解的性质, 其中p, q>2, α, β ≥ 1, a, b> 0是常数. 该文指出上述方程组的解是否在有限时刻爆破依赖于初值、系数 a 与 b以及 αβ 和 (p-1)(q-1)之间的关系.  相似文献   

5.
给出下列具粘性拟线性波方程初边值问题解的能量衰减估计u_(tt)(t,x)-div{σ(|▽u(t,x)|~2)▽u(t,x)}-△u(t,x)-△ut(t,x)+δ|u_t(t,x)|~(p-1)u_t(t,x)=μ|u(t,x)|~(q-1)u(t,x),x∈Ω,t∈(0,T),u(t,x)|■Ω=0,t∈(0,T),u(0,x)=u_0(x),u_t(0,x)=u_1(x),x∈Ω,其中Ω是R~N(N≥1)中具有光滑边界■Ω的区域,p≥1,q1,δ0,μ0,△表示Laplace算子,▽表示梯度算子和σ(s)是一给定的非线性函数.证明的思想是应用一已知的积分不等式,证明以上初边值问题解的能量衰减估计.  相似文献   

6.
给出了如下的非线性椭圆方程自由边值问题-Δu=λu+(1+ε)u+p,x∈B Rn,u|Ω=μ,∫Ωnu=-M(1)在C[0,1]中的球对称解的存在性.并得到比上述问题更一般的非线性椭圆方程自由边值问题-Δu=h(u),x∈B Rn,u|Ω=μ,∫Ωun=-M,在C[0,1]中的球对称解的存在性,其中B为Rn中的单位球,p>1,λ>0,μ<0,M>0,ε>0;λ,μ,M,ε均为常数,n为正整数.  相似文献   

7.
In this article,we study the initial boundary value problem of generalized Pochhammer-Chree equation u_(tt)-u_(xx)-u_(xxt)-u_(xxtt)=f(u) xx,x ∈Ω,t 0,u(x,0) = u0(x),u t(x,0)=u1(x),x ∈Ω,u(0,t) = u(1,t) = 0,t≥0,where Ω=(0,1).First,we obtain the existence of local W k,p solutions.Then,we prove that,if f(s) ∈ΩC k+1(R) is nondecreasing,f(0) = 0 and |f(u)|≤C1|u| u 0 f(s)ds+C2,u 0(x),u 1(x) ∈ΩW k,p(Ω) ∩ W 1,p 0(Ω),k ≥ 1,1 p ≤∞,then for any T 0 the problem admits a unique solution u(x,t) ∈ W 2,∞(0,T;W k,p(Ω) ∩ W 1,p 0(Ω)).Finally,the finite time blow-up of solutions and global W k,p solution of generalized IMBq equations are discussed.  相似文献   

8.
线性抛物型积分微分方程的扩展混合体积元方法   总被引:2,自引:0,他引:2  
1 引言 考虑线性抛物型积分微分方程初边值问题: {pt(x,t)-▽.{A(x,t)▽p(x,t) +∫t0 B(x,t,τ)▽p(x,τ)dτ}=f(x,t),(x,t)∈Ω×(0,T],(1.1) p(x,0):p0(x), x∈Ω, p(x,t)=0, (x,t)∈(a)Ω×(0,T]. 这里x=(x,y),Ω=(a,b)×(c,d),(e)Ω是区域Ω的边界,p为未知函数,A=(aij)2×2为已知的对称正定矩阵,B=(bij)2×2为已知矩阵,而且aij,bij,(aij)t(i,j=1,2)光滑有界,f∈L2(Ω).  相似文献   

9.
<正> 具临界 Sobolev 指数的非线性椭圆方程的正解存在性汪徐家本文将 Brezis 和 Nirenberg 的结果推广到问题(A)(?)其中 L 为一致椭圆算子,b(x)(?)0,f(x,u)为 u~p 在无穷远点的低阶扰动项.问题(A)的解的存在性强烈地依赖于 α_(ij)(x),b(x)和 f(x,u)的性状.例如对任何有界光滑区域Ω都可找到a_ij(x)∈C(?)使 Lu=u~p 在 H_0~1(Ω)中具有一正解.作者还对一类 f(x,u)证明了下面问题非径向解的存在性:-△u=f(|x|,u),u>0于Ω,u=0于(?)Ω,Ω=B(0,1).  相似文献   

10.
记Ω=(0,1)×(0.τ)为钢锭区域,Ω_τ=(0,T)×Ω,Ω_τ=Ω_1(t)∪Ω_2(t),t∈(0,T),其中Ω_1(t)与Ω_2(t)分别表示液态与固态区域。时刻t时的自由界面由F(t)={(x,z)∈Ω,s(X,Z,t)=0}表示,F=(?)F(t)。 设u=u(X,Z,t)表示温度。作变换后不妨设Ω,(t)上  相似文献   

11.
带非局部源的退化半线性抛物型方程解的爆破   总被引:1,自引:0,他引:1  
该文研究带Dirichlet边界条件的退化半线性抛物型方程:xqut-uxx=∫0af(u)dx,这里q>0.作者证明了局部解的存在唯一性并且得到当初值充分大时解在有限时刻爆破.进而,证明解的爆破点集是整个区间[0,a],这与具有局部源的方程解的性质不同.  相似文献   

12.
We consider an aggregation equation in , d2, with fractional dissipation: ut+(uK*u)=−νΛγu, where ν0, 0<γ<1, and K(x)=e−|x|. We prove a refined blowup criteria by which the global existence of solutions is controlled by its norm, for any . We prove the finite time blowup of solutions for a general class of nonsymmetric initial data. The argument presented works for both the inviscid case ν=0 and the supercritical case ν>0 and 0<γ<1. Additionally, we present new proofs of blowup which does not use free energy arguments.  相似文献   

13.
本文研究弱耗散Camassa-Holm方程的Cauchy问题,由Kato理论得到了局部适定性的结果,证明了解的blowup及整体存在性,并证明了当耗散系数满足适当条件时,整体解具有衰减性质.  相似文献   

14.
In this paper, we investigate a semilinear combustible system $u_t-du_{xx}=v^p, v_t-dv_{xx}=u^q$ with double fronts free boundary, where p ≥ 1, q ≥ 1. For such a problem, we use the contraction mapping theorem to prove the local existence and uniqueness of the solution. Also we study the blowup and global existence property of the solution. Our results show that when pq › 1 blowup occurs if the initial datum is large enough and the solution is global and slow, whose decay rate is at most polynomial if the initial value is suitably large, while when p › 1, q › 1 there is a global and fast solution, which decays uniformly at an exponential rate if the initial datum is small.  相似文献   

15.
In this paper, we investigate a reaction-diffusion equation $u_t-du_{xx}=au+\int_{0}^{t}u^p(x,\tau){\rm d}\tau+k(x)$ with double free boundaries. We study blowup phenomena in finite time and asymptotic behavior of time-global solutions. Our results show if $\int_{-h_0}^{h_0}k(x)\psi_1 {\rm d}x$ is large enough, then the blowup occurs. Meanwhile we also prove when $T^*<+\infty$, the solution must blow up in finite time. On the other hand, we prove that the solution decays at an exponential rate and the two free boundaries converge to a finite limit provided the initial datum is small sufficiently.  相似文献   

16.
17.
We study the semilinear parabolic equation ${u_{t}- \Delta u = u^{p}, u \geq 0}$ on the whole space R N , ${N \geq 3}$ associated with the critical Sobolev exponent p = (N + 2)/(N ? 2). Similarly to the bounded domain case, there is threshold blowup modulus concerning the blowup in finite time. Furthermore, global in time behavior of the threshold solution is prescribed in connection with the energy level, blowup rate, and symmetry.  相似文献   

18.
In this paper, we investigate a free boundary problem of a semilinear combustible system with higher dimension and heterogeneous environment. Such a problem is usually used as a model to describe heat propagation in a two-component combustible mixture in which the free boundary is described by Stefan-like condition. For simplicity, we assume that the environment and solutions are radially symmetric. We use the contraction mapping theorem to prove the local existence and uniqueness of the solution. Also we study the blowup property and the long time behavior of the solution. Our results show that when pq › 1 blowup occurs if the initial datum is large enough and the solution is global and slow, whose decay rate is at most polynomial if the initial value is suitably large, while when p › 1, q › 1 there is a global and fast solution, which decays uniformly at an exponential rate if the initial datum is small.  相似文献   

19.
In this paper, we mainly consider the stability of blowup of solutions for the p-Laplace equation with nonlinear source ${u_t = {div}(|\nabla u|^{p-2}\nabla u) + u^q,\;\;(x,t)\in\mathbb{R}^N \times (0,T)}$ , with the initial value ${u(x,0) = u_0(x) \geq 0}$ , where ${\|u_0 (x)\|_{L^\infty} \leq M}$ and T < ∞ is the blowup time. Under a small oscillation around the radial initial value, we can prove the solution blows up in finite time and obtain the blowup rate estimate of the form ${\|u(\cdot,t)\|_{L^\infty}\leq C(T-t)^{-\frac{1}{q-1}}}$ , where the constant C > 0 is dependent only on N, p, q, and the parameters q and p are expected to be ${p > 2, p-1 < q < \frac{Np}{(N-p)}_+ -1}$ .  相似文献   

20.
We study the Euler-Poisson equations of describing the evolution of the gaseous star in astrophysics. Firstly, we construct a family of analytical blowup solutions for the isothermal case in R2. Furthermore the blowup rate of the above solutions is also studied and some remarks about the applicability of such solutions to the Navier-Stokes-Poisson equations and the drift-diffusion model in semiconductors are included. Finally, for the isothermal case (γ=1), the result of Makino and Perthame for the tame solutions is extended to show that the life span of such solutions must be finite if the initial data is with compact support.  相似文献   

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