非紧空间上折现Hamilton-Jacobi方程粘性解的存在性讨论*

当底空间紧时, 初始函数为连续函数的Lax-Oleinik型粘性解是局部半凹的,所以是相应的Hamilton-Jacobi\ (以下简称为H-J) 演化方程(简称为接触H-J方程)的粘性解.当底空间非紧时, 对于H-J方程和接触H-J方程, 其Lax-Oleinik型解的下确界未必能取到.文章将探讨在非紧空间上, 折现H-J方程粘性解有限性的条件, 并给出了在此假设下粘性解的表达式.     

纵波运动方程的分支分析和行波解

本文应用动力系统分支方法研究纵波运动方程,建立一个与该方程相对应的平面系统,并给出该平面系统的分支相图,最后通过相图中的一些特殊轨道获得方程的精确行波解的参数表示,得出行波解之间的联系.     

Finite Integral Transform Solutions for Free Vibrations of Rectangular Thin Plates With Mixed Boundary Constraints北大核心CSCD

Analytical solutions, with unique research value, can serve as benchmarks for empirical formulas and numerical methods, a tool for rapid parameter analysis and optimization, and a theoretical basis for experimental designs. Conventional analytical methods, e.g., the Lévy solution method, are only applicable to mechanical problems of plates and shells with opposite simply-supported edges, which, however, may fail to obtain analytical solutions for the issues with complex boundary constraints. In recent years, the finite integral transform method for plate and shell problems was developed to deal with non-Lévy-type plates and shells, but it is still infeasible to solve the mixed boundary constrains-induced complex boundary value problems of higher-order partial differential equations. Herein, for the first time, the finite integral transform method was combined with the sub-domain decomposition technique to solve the free vibrations of rectangular thin plates with mixed boundary constraints. The rectangular plate was first divided into 2 sub-domains according to the mixed boundary constraints, and the 2 sub-domains were solved analytically with the finite integral transform method. Finally, the continuity conditions were introduced to obtain the analytical solution of the original problem. Based on the side spot-welded cantilever plates commonly used in engineering, the free vibration problem of a rectangular thin plate with 1 edge subjected to clamped-simply supported constraints and the other 3 edges free, was analyzed. The obtained natural frequencies and mode shapes are in good agreement with those from the finite element method as well as the solutions in literature, thus verifying the accuracy of the proposed method. The solution procedure of the finite integral transform method can be implemented based on the governing equations without any assumption of the solution form. Therefore, this strict analytical method is widely applicable to complex boundary value problems of higher-order partial differential equations for such mechanical problems of plates and shells. © 2023 Editorial Office of Applied Mathematics and Mechanics. All rights reserved.     

脉冲条件下Liénard方程周期解的保持性

本文研究带有脉冲的Lienard方程的周期解的存在性问题.我们通过分析Poincaré映射在脉冲点处的变化特征,利用Poincare-Bohl不动点定理证明:在一串脉冲点于时间轴上具有周期分布特征的情况以及适当的脉冲条件之下,如果位势函数满足Lipschitz条件,而强迫项又是周期函数,则Lienard方程x″+f (x)x′+g(x)=p(t)仍然保持周期解的存在性.另外,我们给出了一个具体的Liénard方程例子,来佐证本文中主要结果的有效性.     

复杂函数求最值 同构处理很奇妙

通过对一道函数压轴题的多种解法,揭示出同构处理法的巧妙,难点是对已知条件中的等式或不等式进行变形,使左右两边式子结构形式完全相同,从而找到同一函数模型,再利用函数的单调性进行处理.     

高考解三角形试题中“算两次”原理的应用举例

“算两次”原理是一个重要的原理,能较好培养学生的发散思维能力.本文中通过角度算两次、长度算两次、面积算两次、位置算两次的方法揭示了“算两次”原理在高考解三角形试题中的应用,提升学生思维品质.     

基于模糊博弈视角的企业联盟“双循环”合作对策研究

企业合作在“双循环”新发展格局下呈现出更多的模糊特征,能否形成稳定的模糊合作格局及持续合作的收益再分配策略成为合作联盟的关注点。将广义模糊超量博弈和模糊凸博弈及其广义解集应用到“双循环”新发展格局下企业联盟合作与收益再分配中,提出最大广义模糊超量博弈模型及其广义模糊谈判集,并基于最大广义模糊超量博弈均衡性的视角,对模糊凸博弈下广义模糊谈判集与核心的等价性质进行论证。研究结果不仅满足了“双循环”新发展格局下合作企业以部分资源参与合作的意愿,及企业联盟模糊凸合作博弈下再分配方案等价性证明需求,而且实现了保留部分收益用于联盟再发展的策略。     

全空间■上双相问题径向解的多解性

该研究涉及以下双相问题-div(|▽u|^p-2▽u+μ(x)|▽u|^q-2▽u)+|u|^p-2u+μ(x)|u|^q-2u=λf(x,u),x∈■,其中10,α(■),α∈(0,1]且f:■满足Carathéodory条件.目的是通过利用抽象的临界点理论来确定参数λ的精确正区间,使该问题允许至少一个或两个非平凡径向对称解.     

用Hirota双线性导数变换求MNLS方程的Rogue波解

修正的非线性薛定谔方程(MNLS方程)与导数非线性薛定谔方程(DNLS方程)是两个紧密相关且完全可积的非线性偏微分方程.该文通过Hirota双线性导数变换方法,首先求得MNLS方程在平面简谐波背景下的空间周期解,即Akhmediev型呼吸子解,再通过长波极限得其Rogue波解.根据简单的参数归零法使之自然地约化为DNLS方程的Rogue波解,并借助于一个积分变换将其变换为Chen-Lee-Liu方程的Rogue波解.文章还简要讨论了MNLS方程和DNLS方程在非局域情形整体解的存在性问题.     

质量临界非齐次薛定谔方程在门槛值处的极限行为

该文研究如下与时间无关的具有吸引相互作用的临界非齐次薛定谔方程-△u+|x|²u-am(x)|u|^4/Nu=μu,in R^N,N≥1,其中a> 0且0 0及适合的0≤g(x)<1,令m(x)=1-λg(x),证明该方程在阈值a=a^*处基态解的存在性,并给出λ→0⁺时基态解的极限行为.这些结论推广了Deng,Guo和Lu^[10,11]的结果.特别地,该文使用了一种直接而更简单的方法得到能量的下界.