一类非线性无穷多点边值问题正解的存在性

运用锥拉伸与锥压缩不动点理论,讨论了一类非线性二阶常微分方程无穷多点边值问题u″+a(t).f(u)=0,t∈(0,1),u(1)=∑a_iu(ζ_i),u′(0)=∑b_iu′(ζ_i)正解的存在性.其中a∈C([0,1],[0,∞)),ζ_i∈(0,1),a_i,b_i∈[0,∞),f∈C([0,∞),[0,∞))并且满足∑a_i<1,∑b_i<1.推广了已有文献中的一些结果.     

四阶奇异微分方程边值问题正解的存在性及多解性

研究四阶微分方程边值问题d4udt4=g(t)f(u(t)),0相似文献   

一类半线性周期问题单侧全局区间分歧和定号解

首先建立一类含不可微非线性项周期问题的单侧全局区间分歧定理.应用上述定理,可以证明一类半线性周期问题主半特征值的存在性.进而,可研究下列半线性周期问题定号解的存在性-x″+q(t)x=αx~++βx~-+ra(t)f(x),0tT,x(0)=x(T),x'(0)=x'(T),其中r≠0是一个参数,q,a∈C([0,T],(0,∞)),α,β∈C[0,T],x~+=max{x,0},x~-=-min{x,0};f∈C(R,R),当s≠0时,sf(s)0成立,并且f0∈[0,∞)且f_∞∈(0,∞)或f_0∈[0,∞]且f_∞=0,其中f0=lim∣s∣→0f(s)/s,f_∞=lim∣s∣→+∞f(s)/s.     

一类二阶奇异微分方程边值问题正解的存在性

研究一类二阶奇异微分方程边值问题■正解的存在性,其中f∈C([0,∞),[0,∞)),c∈C([0,∞),[0,∞)),且h∈C((0,1],[0,∞))在t=0处允许有奇性.运用锥拉伸与压缩不动点定理,证明了当非线性项f在原点和无穷远处分别满足超线性和次线性增长条件时,上述问题至少存在一个正解.所得结果不仅可推广已有工作的相关结果,也为更好地研究这类问题的定性性质提供了理论依据.     

二阶强次线性常微分方程的振动性定理

本文讨论二阶微分方程 (a(t)ψ(x)x)+q(t)f(x)g(x′)=0 (1)的解的振动性质。在方程(1)中,a∈C′([t_0,∞)→(0,∞)),ψ∈C′(R→[0,∞)),q∈C([t_0,∞)→[0,∞))且在任意的区间[t,∞)(t≥t_0)上不恒等于0,f∈C′(R→R),g∈C(R→R)。我们仅考虑方程(1)的可以延拓于[t_0,∞)上的解。在任何无限区间[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,则叫振动的;否则就叫非振动的。     

向量值长 James 型 Banach 空间 J(η,l_p)(1≤p<+∞)

本文考虑向量值长 James Banach 空间.其主要结果是:(1)((Φ_(α,i))_(i∈[0,ω)))_(α∈[0,η))是 l_p-值长 James Banach 空间 J(η,l_p)(1≤p<+∞)的超限基,且对任一元素 F∈J(η,l_p)有F=sum α∈[0,η] sum i∈[0,ω) C_(α,i)Φ_(α,i), 其中C_(α,i)=F_(α+1,i)-F_(a,i),(?)α∈[0,η],r∈[0,η],i∈[0,ω),{e_i}_(i∈[0,ω))是 l_p 内的单位向量全体.若 X 是具有 Schauder 基的 Banach 空间,则对于空间 J(η,X)有类似的结论.(2)与 Banach 空间 J(η,l_p)(1相似文献   

二阶测度链上Sturm-Liouville型边值问题的多个正解存在性

本文讨论一类二阶测度链上Sturm-Liouville型边值问题X~△△ f(t,x(σ(t))=0,t∈[t_1,t_2],αx(t_1)—βx~△(t_1)=0,γx(σ(t_2)) δx~△(σ(t_2))=0,其中f_1,t_2](?),(?)是测度链．在适当的条件下,通过运用Leggett-Williams不动点定理,得到了三个正解的存在性．     

一阶线性时超微分不等式

研究了一阶线性时超微分不等式x'(t)-p(t)x(t r)≥0正解的不存在性,其中p(t)∈C([t_0,∞),[0,∞)),T∈R~ 。     

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.     

Positive solutions to m-point boundary value problem of fractional differential equation

In this paper, we study the multiplicity of positive solutions to the following m-point boundary value problem of nonlinear fractional differential equations: Dqu(t) + f(t, u(t)) = 0, 0 < t < 1, u(0) = 0, u(1) =sum (μiDpu(t)|t = ξi ) from i =1 to ∞ m-2, where q ∈R , 1 相似文献   

Lifespan of solutions of semilinear wave equations in two space dimensions

This paper studies the Cauchy problem for some doubly nonlinear degenerate parabolic equations (1.1) with initial data (1.2). Hölder continuous solutions, with explicit Hölder exponents uniformly in [0,T] * R^N for any given time T, are obtained by using the maximum principle.     

Reaction diffusion equations with non-linear boundary conditions,blowup and steady states

In this paper we study the following problem: u_t−Δu=−f(u) in Ω×(0, T)≡Q_T, ∂u ∂n=g(u) on ∂Ω×(0, T)≡S_T, u(x, 0)=u₀(x) in Ω , where Ω⊂ℝ^N is a smooth bounded domain, f and g are smooth functions which are positive when the argument is positive, and u₀(x)>0 satisfies some smooth and compatibility conditions to guarantee the classical solution u(x, t) exists. We first obtain some existence and non-existence results for the corresponding elliptic problems. Then, we establish certain conditions for a finite time blow-up and global boundedness of the solutions of the time-dependent problem. Further, we analyse systems with same kind of boundary conditions and find some blow-up results. In the last section, we study the corresponding elliptic problems in one-dimensional domain. Our main method is the comparison principle and the construction of special forms of upper–lower solutions using related equations. © 1998 B. G. Teubner Stuttgart—John Wiley & Sons, Ltd.     

The Strong Solution of a Class of Generalized Navier-Stokes Equations

We study initial boundary value (lBV) problem for a class of generalized Navier-Stokes equations in L^q([0, T); L^p(Ω)). Our main tools are regularity of analytic semigroup by Stokes operator and space-time estimates. As an application we can obtain some classical results of the Navier-Stokes equations such as global classical solution of 2-dimensional Navier-Stokes equation etc.     

时间尺度上三阶Emden-Fowler动力方程的振动准则

运用Riccati 变换技术, 研究了时间尺度T上三阶Emden-Fowler时滞动力方程 (a(t)(r(t)x^? (t))^? ) ^?+p(t)x^γ(τ(t)) = 0 的振动性, 这里γ>0是正奇数的比, a, r, p是定义在T上的正的实值rd -连续函数. 得到一些新的振动结果, 推广和丰富了已有文献中的结论. 另外, 还给出了几个例子说明主要结果的合理性.     

一个带非线性边界条件的强耦合抛物方程组的整体存在性与爆破

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     

Interfacial phenomenon for one-dimensional equation of forward-backward parabolic type

Summary An interfacial phenomenon for a class of the solutions of a nonlinear forward-backward parabolic equation in R × (0,T) is investigated. In general, short time-period of interfaces is considered. This inner analysis allows to construct on some time interval a solution of the Cauchy problem for certain initial data.     

Interval length continuation method for solving two-point boundary-value problems

We consider the solution of the following two-point boundary-value problem: $$\begin{gathered} \dot x(t) = f(t,x(t),p(t)), \dot p(t) = g(t,x(t),p(t)), t \in [0,T], \hfill \\ h(x(0),p(0)) = 0, p(T) = q. \hfill \\ \end{gathered} $$ We propose a combination technique consisting of the interval length continuation method and the back-and-forth shooting method. Certain alternative ways of employing continuation are discussed, and some of them are well suited for the problem under consideration. As a test for the method, a numerical example of a problem originating in optimal control is given.     

On the Cauchy Problem and Initial Trace for Nonlinear Filtration Type with Singularity

In this paper, we consider the Cauchy problem \frac{∂u}{∂t} = Δφ(u) in R^N × (0, T] u(x,0} = u_0(x) in R^N where φ ∈ C[0,∞) ∩ C¹(0,∞), φ(0 ) = 0 and (1 - \frac{2}{N})^+ < a ≤ \frac{φ'(s)s}{φ(s)} ≤ m for some a ∈ ((1 - \frac{2}{n})^+, 1), s > 0. The initial value u_0 (z) satisfies u_0(x) ≥ 0 and u_0(x) ∈ L¹_{loc}(R^N). We prove that, under some further conditions, there exists a weak solution u for the above problem, and moreover u ∈ C^{α, \frac{α}{2}}_{x,t_{loc}} (R^N × (0, T]) for some α > 0.     

奇异半线性发展方程的局部Cauchy问题

本文在Ｂａｎａｃｈ空间Ｅ中讨论如下问题ｄｕｄｔ＋１ｔσＡｕ＝Ｊ（ｕ），０＜ｔＴ，ｌｉｍｔ→０＋ｕ（ｔ）＝０，其中ｕ：（０，Ｔ］Ｅ，Ａ是与ｔ无关的线性算子．（－Ａ）是Ｅ上Ｃ０半群｛Ｔ（ｔ）｝ｔ０的无穷小生成元，常数σ１，Ｊ是一个非线性映射ＥＪ→Ｅ．它满足局部Ｌｉｐｓｃｈｉｔｚ条件．我们证明了当其Ｌｉｐｓｃｈｉｔｚ常数ｌ（ｒ）满足一定条件时．问题（Ｓ）有局部解，且在某函类中解唯一．设Ｊ（ｕ）＝｜ｕ｜γ－１ｕ＋ｆ（ｘ）（γ＞１），Ｅ＝Ｌｐ，ＥＪ＝Ｌｐγ时得到了与Ｗｅｉｓｌｅｒ［２］在非奇异情形类似的结果．