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   

四阶边值问题正解的存在性与多解性

本文讨论了非线性四阶边值问题u^(4)(t)=φ（t）f(u(t),u“(t),t∈(0,1),u(0)=u(1)=u“(0) =u“(1)=0正确的存在性，其中φ（t)∈C([0,1],[0,∞)),f(u,v)∈C（[0,∞],[0,∞))。利用锥压缩与锥拉伸不动点定理，给出了该问题正解存在与多个正解存在的充分条件。     

一阶微分方程的渐近平稳和周期边值问题

假定函数 f∈C[R_+×R,R],我们考虑非线性问题u'=f(t,u),u(t_0)=u_0,t_0≥0.(A)[1]附录的定理 A.1.2就(A)的渐近平稳(Asymptotic Equilibrium)给出如下的定理 A。假定 g(t,u)∈C[R_+×R_+,|R_+]对于每个 t 关于 u 单调非减,且使得|f(t,u)|≤g(t,|u|),(t,u)∈R_+×R.如果问题u′=g(t,u),u(t_0)=u_0≥0的所有解 u(t)在[t_0,∞)上有界,那么问题(A)渐近平稳.利用这个定理,[1]在假定,f(t,u)满足单边的 Lipschitz 条件     

一个奇异典型弹性梁方程涉及第一特征值的正解

本文研究非线性四阶边值问题u(4)(t)=f(t,u(t)),0π4/16;(ii)∫10lim inf x→+0f(t,x)/x dt>π4/16并且∫10lim sup x→+∞f(t,x)/x dt<π4/16.     

Sobolev方程的基于H~1-Galerkin混合方法的新分裂格式

正1引言考虑如下Sobolev方程u_t-▽·(a(x)▽u_t+a(x)▽u)+u=f(x,t),(x,t)∈Ω×J,u(x,t)=0,(x,t)∈аΩ×J,(1)u(x,0)=u_0(x),x∈Ω.其中Ω是R~d(d=1,2,3)中具有边界     

奇异二阶Neumann边值问题的正解

考察非线性二阶边值问题-u″(t)+λu(t)=h(t)f(t,u(t))+ζ(t,u(t)),0＜t＜1,u′(0)=u′(1)=0,的正解,其中λ＞0.文中允许ζ(t,u)在t=0,t=1和u=0处奇异.利用锥上的Guo-KraLsnosel'skii不动点定理证明了n个正解的存在性,其中n是任意的正整数.     

四阶微分方程的迭代解

利用一个构造性的方法,在假设边值问题存在上解α和下解β,满足β≤α的前提下,给出了两个单调序列它们一致收敛于如下两类边值问题的极值解u(4)(x)-Mu″(x)=f(x,u(x),u'(x),u″(x),u″'(x)),0＜x＜1,u(0)=u'(1)=u″(0)=u″'(1)=0;u(4)(x)-Mu″(x)=g(x,u(x),u'(x),u″(x)),0＜x＜1,u(0)=u'(1)=u″(0)=u″'(1)=0.     

奇数阶边值问题正解的存在性与多重性

利用锥拉伸锥压缩不动点定理,证明了在一定条件下,下列非线性奇数阶方程(-1)q+1u(2q+1)(t)=λa(t)f(u(t)),0 t 1,(-1)q+1u(2q+1)(t)=λa(t)f(u(t)),0 t 1,u(0)=u′(τ)=u″(1)=0u(2j+1)(0)=u(2j+1)(1)=0,j=1,2,…,q-1.单个和多个正解的存在性,其中λ>0,12<τ<1,q∈N.得到了λ的区间Λ,对一切λ∈Λ,该问题至少有一个正解,同样也得到了该问题至少有两个正解λ相应的区间.     

三阶微分方程组边值问题常号解的存在性

利用Krasnoselskii不动点定理,结合Leray-Schauder度,研究下列三阶微分方程组边值问题{ui″′(t)=fi(t,u1(t),u2(t),u3(t)), t∈[0,1],/ui′(0)=ui″(0)=ui(1)=0, i=1,2,3. 在某些条件下,常号解的存在性和多解性.     

一类奇异半线性反应扩散方程初值问题解的存在性

本文获得了如下的奇异半线性反应扩散方程初值问题{(e)u/(e)t-(1/tσ)△u=up+f(x),t＞0,x∈Rnlim t→0+ u (t,x)=0, x∈Rn广义解(mild solution)在L∞ loe[(0,∞);L∞(Rn)]中的存在性.其中σ＞0,0＜p＜1,f(x)非负且f(x)∈L∞(Rn).     

Positive solution for fourth-order m-point nonhomogeneous boundary value problems

This paper is concerned with the following fourth-order m-point nonhomogeneous boundary value problem $$\begin{array}{l}u^{(4)}(t)=f(t,u(t),u^{\prime \prime }(t)),\quad 0<t<1,\\[3pt]u(0)=u(1)=u^{\prime \prime }(0)=0,\\[3pt]u^{\prime \prime }(1)-\displaystyle\sum_{i=1}^{m-2}a_{i}u^{\prime\prime }(\xi _{i})=-\lambda ,\end{array}$$ where a _i ≥0 (i=1,2,…,m?2), 0<ξ₁<ξ₂<???<ξ _m?2<1 and ∑ _i=1 ^m?2 a _i ξ _i <1, and λ>0 is a parameter. The existence and nonexistence of positive solution are discussed for suitable λ>0 when f is superlinear or sublinear. The main tool used is the well-known Guo-Krasnoselskii fixed point theorem.     

具$p$-Laplacian 算子的多点边值问题迭代解的存在性

利用单调迭代技巧和推广的Mawhin定理得到下述带有p-Laplacian算子的多点边值问题迭代解的存在性,{(Фp(u'))' f(t,u, Tu)=0, 0(≤)t(≤)1,u(0)=q-1∑i=1γiu(δi),u(1)=m-1∑i=1ηiu(ξi),其中Фp(s)=|s|p-2s,p＞1;0＜δi＜1,γi＞0,1(≤)i(≤)q-1;0＜ξi＜1,ηi(≥)0,1(≤)i(≤)m-1且q-1∑i=1γi＜1,m-1∑i=1ηi(≤)1;Tu(t)=∫t0k(t,s)u(s)ds,k(t,s)∈C(I×I,R ).     

Asymptotic Behavior of Positive Solutions of a Nonlinear Combined p-Laplacian Equation

For p > 1, we establish existence and asymptotic behavior of a positive continuous solution to the following boundary value problem $$\left\{\begin{array}{ll}\frac{1}{A} \left( A\Phi _{p}(u^{\prime})\right) ^{\prime}+a_{1}(r)u^{\alpha _{1}}+a_{2}(r)u^{\alpha _{2}}=0, \, {\rm in}\, (0,\infty ),\\ {\rm lim}_{r\rightarrow 0} A\Phi _{p}(u^{\prime})(r)=0, {\rm lim}_{r\rightarrow \infty } u(r)=0,\end{array}\right.$$ where \({\alpha _{1}, \alpha _{2} < p -1, \Phi _{p}(t) = t|t| ^{p-2},A}\) is a positive differentiable function and a ₁, a ₂ are two positive functions in \({C_{\rm loc}^{\gamma}((0, \infty )), 0 < \gamma < 1,}\) satisfying some appropriate assumptions related to Karamata regular variation theory. Also, we obtain an uniqueness result when \({\alpha _{1}, \alpha _{2} \in (1-p,p-1)}\) . Our arguments combine a method of sub and supersolutions with Karamata regular variation theory.     

Continuous dependence on the boundary conditions for the Wentzell Laplacian

The solution u of the well-posed problem

Existence of at least three positive solutions for multi-point boundary value problem on infinite intervals with p-Laplacian operator

In this paper, we consider the multi-point boundary value problem of second-order nonlinear differential equation on a half line, $$\left\{\begin{array}{l@{\quad }l}(\phi_{p}(u'))'(t)+q(t)f(t,u(t),u'(t))=0,&0<t<\infty,\\[6pt]u'(0)=\sum_{i=1}^{m-2}\alpha_{i}u(\xi_{i}),&u'(\infty)=0.\end{array}\right.$$ By using a fixed point theorem due to Avery and Peterson, we show the existence of at least three positive solutions with suitable growth conditions imposed on the nonlinear term.     

Positive solutions for a boundary-value problem with Riemann–Liouville fractional derivative*

In this work, we are mainly concerned with the existence of positive solutions for the fractional boundary-value problem $$ \left\{ {\begin{array}{*{20}{c}} {D_{0+}^{\alpha }D_{0+}^{\alpha }u=f\left( {t,u,{u}^{\prime},-D_{0+}^{\alpha }u} \right),\quad t\in \left[ {0,1} \right],} \hfill \\ {u(0)={u}^{\prime}(0)={u}^{\prime}(1)=D_{0+}^{\alpha }u(0)=D_{0+}^{{\alpha +1}}u(0)=D_{0+}^{{\alpha +1}}u(1)=0.} \hfill \\ \end{array}} \right. $$ Here ?? ?? (2, 3] is a real number, $ D_{0+}^{\alpha } $ is the standard Riemann?CLiouville fractional derivative of order ??. By virtue of some inequalities associated with the fractional Green function for the above problem, without the assumption of the nonnegativity of f, we utilize the Krasnoselskii?CZabreiko fixed-point theorem to establish our main results. The interesting point lies in the fact that the nonlinear term is allowed to depend on u, u??, and $ -D_{0+}^{\alpha } $ .     

General decay and blow-up of solutions for a viscoelastic equation with nonlinear boundary damping-source interactions

In this paper, a viscoelastic equation with nonlinear boundary damping and source terms of the form $$\begin{array}{llll}u_{tt}(t)-\Delta u(t)+\displaystyle\int\limits_{0}^{t}g(t-s)\Delta u(s){\rm d}s=a\left\vert u\right\vert^{p-1}u,\quad{\rm in}\,\Omega\times(0,\infty), \\ \qquad\qquad\qquad\qquad\qquad u=0,\,{\rm on}\,\Gamma_{0} \times(0,\infty),\\ \dfrac{\partial u}{\partial\nu}-\displaystyle\int\limits_{0}^{t}g(t-s)\frac{\partial}{\partial\nu}u(s){\rm d}s+h(u_{t})=b\left\vert u\right\vert ^{k-1}u,\quad{\rm on} \ \Gamma_{1} \times(0,\infty) \\ \qquad\qquad\qquad\qquad u(0)=u^{0},u_{t}(0)=u^{1},\quad x\in\Omega, \end{array}$$ is considered in a bounded domain ??. Under appropriate assumptions imposed on the source and the damping, we establish both existence of solutions and uniform decay rate of the solution energy in terms of the behavior of the nonlinear feedback and the relaxation function g, without setting any restrictive growth assumptions on the damping at the origin and weakening the usual assumptions on the relaxation function g. Moreover, for certain initial data in the unstable set, the finite time blow-up phenomenon is exhibited.     

Existence Theory for an Arbitrary Order Fractional Differential Equation with Deviating Argument

In this paper, we are concerned with the existence criteria for positive solutions of the following nonlinear arbitrary order fractional differential equations with deviating argument

A note on a fourth order degenerate parabolic equation in higher space dimensions

We are concerned with existence, positivity property and long-time behavior of solutions to the following initial boundary value problem of a fourth order degenerate parabolic equation in higher space dimensions      

Infinitely Many Solutions for Systems of Sturm–Liouville Boundary Value Problems

In this paper, the authors obtain the existence of infinitely many classical solutions to the boundary value system with Sturm–Liouville boundary conditions $$\left\{\begin{array}{ll}-(\phi_{p_i}(u_{i}^\prime))^\prime = \lambda F_{u_{i}}(x,u_{1},\ldots,u_{n})h_{i}(u^\prime_i)\quad {\rm in} \, (a,b), \\ \alpha_iu_{i}(a)-\beta_iu^ \prime_{i}(a)=0, \quad \gamma_iu_{i}(b)+\sigma_iu^\prime_{i}(b)=0, \end{array}\quad{i = 1, \ldots , n.} \right.$$ Critical point theory and Ricceri’s variational principle are used in the proofs.