分数阶趋化模型在临界Besov空间中解的整体存在性北大核心CSCD

该文主要研究如下的分数阶趋化模型:{■_(t)+(-△)^(α/2)=▽·(u▽v)(x,t)∈R^(n)×(0,∞),ε■_(t)v+(-△)^(β/2)v=u,(x,t)∈R^(n)×(0,∞),u(x,0)=u_(0)(x),v(x,0)=v_(0)(x),x∈R^(n)其中α∈[1,2],β∈(0,2],ε≥0.基于分数阶耗散方程在Chemin-Lerner混合时空空间中的线性估计和Fourier局部化方法,作者得到了如下结果:(1)当ε=0时,建立了次临界情形1<α≤2下该模型在Besov空间中的局部适定性和小初值问题的整体适定性,优化了[陈化,吕文斌,吴少华.分数阶趋化模型在Besov空间中解的存在性.中国科学:数学,2019,49(12):1-17]所得适定性结果中正则性和可积性指标的范围.并且还建立了临界情形α=1下该模型在Besov空间中小初值问题的整体适定性;(2)当ε>0时,利用特殊的迭代技巧,作者分别建立了次临界情形1<α≤2和临界情形α=1下该模型在Besov空间中的局部适定性和小初值问题的整体适定性.进一步,利用模型所特有的代数结构,作者还证明了对初值v0无小性条件下解的整体存在性.     

奇摄动半线性时滞微分方程边值问题

本文研究半线性时滞微分方程边值问题εx″(t) =f (t,x(t) ,x(t-ε) ,ε) ,t∈ (0 ,1 ) ,x(t) =φ(t,ε) ,t∈ [-ε,0 ],x(1 ) =A(ε) .利用不动点原理及微分不等式理论 ,我们证明了边值问题解的存在性 ,并给出了解的一致有效渐近展开式 .     

具非线性边界条件的泛函微分方程边值问题奇摄动(英文)

研究一类具非线性边界条件的泛函微分方程边值问题εx″( t) =f ( t,x( t) ,x( t-τ) ,x′( t) ,ε) ,　 t∈ ( 0 ,1 ) ,x( t) =φ( t,ε) ,　 t∈ [-τ,0 ],　 h( x( 1 ) ,x′( 1 ) ,ε) =A(ε) .我们利用微分不等式理论证明了边值问题解的存在性 ,并给出了解的一致有效渐近展开式     

二阶哈密尔顿系统的对称扰动(英文)

我们研究二阶Hamiltonian系统-ü=▽F1(t,u)+ε▽F2(t,u)a.e.t∈[0,T]的多重周期解,其中ε是一个参数,T0.F1(F2)∶R×RN→R关于t是T周期的,▽F1(t,x)关于x是奇的;并且Fi(t,x)(i=1,2)对所有x∈RN关于t是可测的,对几乎所有t∈[0,T]关于x是连续可微的,而且存在a∈C(R+,R+),b∈L+(0,T;R+)使得|Fi(t,x)|≤a(|x|)b(t),|▽Fi(t,x)|≤a(|x|)b(t)对所有x∈RN及几乎所有t∈[0,T]成立.我们对F1施加适当的条件,能够证明对任意的j∈N存在εj0使得|ε|≤εj,则上述问题至少有j个不同的周期解.     

二阶非线性阻尼常微分方程的振动性定理

考虑二阶非线性阻尼微分方程(α(t)ψ(x(t))x′(t))′ p(t)x′(t) q(t)f(x(t))=0 (1)和二阶非线性微分不等式x(t){(α(t)ψ(x(t))x′(t))′ p(t)x′(t) q(t)f(x(t))}≤0,(2)其中α,p,q∈C([t_0,∞)→(-∞,∞)),ψ,f∈C(R→R),并且α(t)>0,xf(x)>0 (x≠0).此外,我们总假设方程(1)的每一个解 x(t)可以延拓于[t_0, ∞)上.在任何无穷区间[T,∞)上,x(t)不恒等于零,这样的解叫正则解.一个正则解,若它有任意大的零点,则称为振动的;否则就称为非振动的.若方程(1)的所有正则解是振动的,则称方程(1)是振动的.关于不等式(2)的振动性的定义,与方程(1)的振动性的定义完全类似,不再赘述.     

一类具有转向点的三阶微分方程的边值问题的解的高阶渐近展开

利用上下解方法,研究如下一类具有转向点的三阶微分方程的边值问题{ε~2y″′=f(t,y,ε)y″ g(t,y,ε)y′ h(t,y,ε),a相似文献   

算子与边界双摄动的非线性方程边值问题的奇摄动

本文应用在边界层构造校正项的方法研究算子与边界摄动相结合的二阶非线性边值问题εx″=g(t,x,ε),μ≤t≤1-μx(t,ε)|_(t-μ)=α(ε,μ)x(t,ε)|_(t-1-μ)=β(ε,μ)的奇摄动,导出解及其导函数的一致有效渐近式和余项的估计,并证明当小参数是充分小时,边值问题的解是存在和唯一.     

凸区域上拟线性椭圆型方程的尖峰解

本文讨论奇异扰动的拟线性椭圆型方程-ε△pu(x)=f(u(x)),u(x)≥0,x∈Ω;u=0,x∈Ω在Dirichlet边值条件下极小能量解的存在性和结构.其中ε＞0是小参数,p＞2,△pu=div(|Du|p-2Du),f(s)=sq-sp-1,p-1＜q＜Np/N-p-1.Ω RN(N≥2)是有界光滑区域.当ε→0时,方程存在一个极小能量解,应用移动平面方法可以证明此解在凸区域上会变成一个尖峰解.     

非线性向量边值问题的奇异摄动

本文研究摄动边值问题dx/dt=f(x,y,t;ε),εdy/dt=g(x,y,t;ε),a_1(ε)x(0,ε)+a_2(ε)y(0,ε)=a(ε)b_1(ε)x(1,ε)+εb_2(ε)y(1,ε)=β(ε)这里x,f,β∈E~m,y,g,a∈E~n,0<ε《1,a_1(ε),a_2(ε),b_1(ε),b_2(ε)为适当阶数的矩阵.在g_y(t)是非奇异矩阵及其它的适当限制下,证明了解的存在唯一性,作出了解的n阶渐近近似式,并得出余项估计.     

非线性Schrdinger方程基态解的一致集中

本文讨论一类非线性Schrdinger方程-ε~2△v+V(z)v=K(x)v~p,x∈R~N,v∈W~(1,2)(R~N),v(x)>0,势函数V(x)有正下界和在无穷远处为零两种情形.通过强最大值原理我们证明方程的基态解关于充分小的ε>0一致集中.     

半线性抛物型方程组解的整体存在性与爆破速率估计

研究了具有非线性热源的半线性抛物型方程组的齐次neumann问题解的爆破性质.利用上下解方法得到了解整体存在的条件与爆破条件,并利用FriedmannMcleod方法建立了爆破速率估计.     

On the blow‐up phenomena for a 1‐dimensional equation of ion sound waves in a plasma: Analytical and numerical investigation

The initial‐boundary value problem for an equation of ion sound waves in plasma is considered. A theorem on nonextendable solution is proved. The blow‐up phenomena are studied. The sufficient blow‐up conditions and the blow‐up time are analysed by the method of the test functions. This analytical a priori information is used in the numerical experiments, which are able to determine the process of the solution's blow‐up more accurately.     

方程utt-△u-△ut-△utt=f(u)的初边值问题

本文研究一类四阶非线性耗散、色散波动方程的初边值问题｛ｕｔｔ－△ｕ－△ｕｔ－△ｕｔｔ＝ｆ（ｕ）,ｕ│ｔ＝０＝ｕ０（ｘ）,ｕｔ│ｔ＝０＝ｕ１（ｘ）,ｕ│эΩ＝０,得到了问题整体强解的存在性和唯一性,并在一定条件下,研究了解的渐近性质和ｂｌｏｗ ｕｐ现象。     

一类非线性扩散方程解的blow up速率估计

利用F riedm an-M cleod方法和变动尺度方法研究了一类具有非线性边界条件的非线性扩散方程解的b low up问题,证明了解在有限时间b low up,并且得到了b low up速率估计.     

Numerical methods for a coupled system of differential equations arising from a thermal ignition problem

This article is concerned with monotone iterative methods for numerical solutions of a coupled system of a first‐order partial differential equation and an ordinary differential equation which arises from fast‐igniting catalytic converters in automobile engineering. The monotone iterative scheme yields a straightforward marching process for the corresponding discrete system by the finite‐difference method, and it gives not only a computational algorithm for numerical solutions of the problem but also the existence and uniqueness of a finite‐difference solution. Particular attention is given to the “finite‐time” blow‐up property of the solution. In terms of minimal sequence of the monotone iterations, some necessary and sufficient conditions for the blow‐up solution are obtained. Also given is the convergence of the finite‐difference solution to the continuous solution as the mesh size tends to zero. Numerical results of the problem, including a case where the continuous solution is explicitly known, are presented and are compared with the known solution. Special attention is devoted to the computation of the blow‐up time and the critical value of a physical parameter which determines the global existence and the blow‐up property of the solution. © 2012 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq 2013     

Global existence and bounds for blow‐up time in a class of nonlinear pseudo‐parabolic equations with a memory term

In this article, we consider the initial boundary value problem for a class of nonlinear pseudo‐parabolic equations with a memory term: Under suitable assumptions, we obtain the local and global existence of the solution by Galerkin method. We prove finite‐time blow‐up of the solution for initial data at arbitrary energy level and obtain upper bounds for blow‐up time by using the concavity method. In addition, by means of differential inequality technique, we obtain a lower bound for blow‐up time of the solution if blow‐up occurs.     

退化的抛物方程组解的全局存在及爆破

本文讨论了退化抛物方程组初边值问题解的性质 ,通过构造上、下解 ,证明了古典解的存在唯一性 ,利用特征函数以及最大值原理 ,得出了解全局存在以及爆破的若干条件 .     

Blow‐up behavior of the Solution for the problem in a subdiffusive mediums

The diffusion problem in a subdiffusive medium is formulated by using the fractional differential operator. In this paper, we consider a fractional differential equation with concentrated source. The existence of the solution in a finite time is given. The finite time blow‐up criteria for the solution of the problem is established, and the location of the blow‐up point is investigated.     

非线性Sobolev-Galpern方程解的blow up

本文研究非线性Ｓｏｂｏｌｅｖ－Ｃａｌｐｅｒｎ方程的初边值问题整体解的不存性即解的爆破问题,用能量估计方法并借助于Ｊｅｎｓｅｎ不等式证明了非线性Ｓｏｂｏｌｉｖ－Ｇａｌｐｅｒｎ方程各种初边值问题在某些假设下不存在整体解。     

Numerical Study of Blow‐Up Mechanisms for Davey–Stewartson II Systems

We present a detailed numerical study of various blow‐up issues in the context of the focusing Davey–Stewartson II equation. To this end, we study Gaussian initial data and perturbations of the lump and the explicit blow‐up solution due to Ozawa. Based on the numerical results it is conjectured that the blow‐up in all cases is self‐similar, and that the time‐dependent scaling behaves as in the Ozawa solution and not as in the stable blow‐up of standard L ² critical nonlinear Schrödinger equation. The blow‐up profile is given by a dynamically rescaled lump.