边界阻尼力对复合材料层合板主参激共振的影响

结合经典层合板理论与von Kármán理论并利用Galerkin截断,获得受面内激励具边界阻尼力的四边铰支正交对称铺设矩形层合薄板的动力学控制方程。基于多尺度法,形成了确定性激励下系统主参激共振的近似解析形式,结果表明:系统平凡响应不稳定区间带宽只与线性阻尼及激励幅值有关,而边界阻尼力的大幅增加可有效减小主参激共振时非平凡响应的幅值及共振频率范围。随后,将确定性激励扩展为窄带随机激励,结合所得Foker-Planck-Kolmogorov方程并采用有限差分法,数值分析了系统稳态响应在平凡与非平凡解支间的随机跳跃现象,结果表明:微小的边界阻尼力增量,将导致系统的稳态响应从非平凡解支跳向平凡解支。     

微分差分方程解的渐近稳定性

本文不同于文[1-5]的方法,从另外的角度研究了一类非线性微分差分方程零解的渐近稳定性,得到了充分条件.另外,本文考虑了特征方程具有零根的时变线性微分差分方程平凡解的渐近稳定性,得到了渐近稳定的充分条件,从而说明了对于时变线性微分差分系统,其特征方程根均具有负实部不是系统平凡解渐近稳定的必要条件。     

直线运动柔性梁非线性动力学--组合参数共振与内共振联合激励

针对基础直线运动柔性梁，基于Kane方程建立了相应的非线性动力学方程。采用多尺度法并结合笛卡尔坐标变换，导出了系统受前两阶模态间3：1内共振及其组合参激共振时的非线性调制方程组，数值求解了该方程组的定常解及相应的稳定性问题。研究表明，系统的平凡响应与双模态非平凡响应共存，由内共振所产生的非平凡响应皆为不稳定的鞍点，平凡及非平凡解分支都存在Hopf分岔现象，一些稳定的极限环随参数变化最终经倍周期分岔后产生混沌运动。     

纵向磁场中导电薄板的亚谐共振

基于麦克斯韦方程和弹性动力学理论,导出了纵向磁场中导电薄板的非线性磁弹性耦合振动方程和电动力学方程,运用伽辽金法推得了两对边简支导电条形板的达芬型振动方程.针对亚谐波共振问题,应用多尺度法进行求解,得到了相应的近似解析解和幅频响应方程以及非平凡解存在条件.应用李雅普诺夫稳定性理论,对解的稳定性进行了分析,得到了稳态解稳...     

具有非平凡零空间的第二类Fredholm积分方程的有限元解

本文利用线性算子理论中的一些结果,讨论了具有非平凡零空间的第二类Frcdholm积分方程的数值解,给出了正则化解和有限元正则化解的表达式,并得到了近似解的误差估计。     

关于一个半线性椭圆方程解的存在性定理

证明一个关于方程-△u=|u|p-1u非平凡解的存在性的定理,拓宽了现有的定理.     

一类椭圆型方程非线性边值问题解的存在性

讨论了具有Sobolev临界指数的一类拟线性椭圆型方程非平凡解的存在性，利用集中紧原理得到了一个存在性结果。     

含时滞的半线性反应扩散方程解的L2一致渐近稳定性

采用两个Lyapunov泛函方法研究含时滞的时变半线性反应扩散方程,得到其平凡解L^2一致渐近稳定的充分性判别定理。     

一类二阶非线性差分方程的振动性质

从解的渐近状态着手,将所述方程的所有非平凡解分成互不相交的四类,应用分类讨论方法和分析方法,讨论了一类广泛的二阶非线性差分方程解的振动性质,建立了两个新的振动性定理,推广并改进了已有文献中的相关结果。     

Klein-Gordon-Maxwell系统解的存在性和多解性

Klein-Gordon-Maxwell系统具有很强的物理背景,它提供了带电粒子物质和它所产生的电磁场之间作用的“二元模型”描述．根据这个模型,粒子物质是一个非线性场方程的孤波解,且电磁场的作用是由场方程与麦克斯韦方程耦合的衡量电位描述的．本文利用变分方法和临界点理论研究一类Klein-Gordon-Maxwell系统解的存在性和多重性．首先,利用山路引理,我们证明了系统非平凡解的存在性,其中一个解是非负的,一个解是非正的．其次,运用喷泉定理,文中证明系统在非线性项满足一定条件下无穷多高能量解的存在性．本文所得结果推广了以前的结论．     

关于扰动差分方程零解的稳定性

讨论了一类扰动差分方程组零解的稳定性，一致稳定性，全局渐近稳定性及全局一致渐近稳定性。     

Spatio-temporal pattern formation in a nonlocal reaction-diffusion equation

We study a scalar reaction-diffusion equation which contains a nonlocal term in the form of an integral convolution in the spatial variable and demonstrate, using asymptotic, analytical and numerical techniques, that this scalar equation is capable of producing spatio-temporal patterns. Fisher's equation is a particular case of this equation. An asymptotic expansion is obtained for a travelling wavefront connecting the two uniform steady states and qualitative differences to the corresponding solution of Fisher's equation are noted. A stability analysis combined with numerical integration of the equation show that under certain circumstances nonuniform solutions are formed in the wake of this front. Using global bifurcation theory, we prove the existence of such non-uniform steady state solutions for a wide range of parameter values. Numerical bifurcation studies of the behaviour of steady state solutions as a certain parameter is varied, are also presented.     

具有阶段结构和时滞比率依赖的捕食系统的持续生存和稳定性

本文研究了一类带有时滞和对捕食者进行分阶段的比率依赖的捕食模型,得到了该模型中的种群的持续生存的充分条件。通过构造Lyapunov泛函的方法,得到了该模型唯一正平衡点的局部稳定和全局稳定的充分条件。     

带B-D反应项的捕食-食饵模型正解的一致持续性

本文利用上下解方法和稳定性理论,讨论了一类带Beddington-DeAngelis反应项的捕食.食饵模型解的渐近行为,给出了正解一致持续的充分条件.同时,利用上下解方法证明了一个正的全局吸引子的存在性.文中的结果表明,在一定的条件下,相互作用的种群是可以持续生存的.     

Critical study of existing solutions for a penny-shaped interface crack, comparing with a new boundary element solution allowing for frictionless contact

A numerical study of the fundamental problem of a pressurized penny-shaped crack at the interface of two dissimilar half spaces is carried out allowing for the possibility of frictionless contact between crack faces. A new, highly accurate axi-symmetric formulation of the boundary element method (BEM) for the solution of elastic contact problems is employed. The correctness and accuracy of available predictions of different kinds for several key characteristics of the solution of this problem are checked. First, comparison of the BEM results for the near-tip contact length shows a very good agreement with some existing predictions. Second, the global solution obtained by BEM is compared with existing asymptotic solutions, obtained with both the open and the frictionless contact models. BEM results show that at the closest neighborhood to the crack tip the global solution of the problem is governed by the first term of the asymptotic solution of the frictionless contact model (up to a distance of the order of a fraction of the near-tip contact length). After a small transition region, in an adjacent surrounding zone whose extent is almost independent of the near-tip contact length, the global solution of the problem is governed by the first term of the asymptotic solution of the open model. As a result of the comparison presented, the regions in which the classical fracture parameters, stress intensity factor (SIF) and energy release rate, can be accurately obtained from the global numerical solution of a crack of this kind have been determined. Third, BEM results and previous estimations show certain discrepancies with a recently published closed form solution of the near-tip contact length and the mode II SIF of the frictionless contact model. A new closed form expression of this mode II SIF, derived from the asymptotic solution of the open model, is proposed in this paper.     

Long-time behaviour of multi-component fluid mixtures in porous media

The long-time behaviour of a triply convective-diffusive fluid mixture saturating a porous horizontal layer in the Darcy-Oberbeck-Boussinesq scheme, is investigated. It is shown that the L²- solutions are bounded, uniquely determined (by the initial and boundary data) and asymptotically converging toward an absorbing set of the phase-space. The stability analysis of the conduction solution is performed. The linear stability is reduced to the stability of ternary systems of O.D.Es and hence to algebraic inequalities. The existence of an instability area between stability areas of the thermal Rayleigh number (“instability island”), is found analytically when the layer is heated and “salted” (at least by one “salt”) from below. The validity of the “linearization principle” and the global nonlinear asymptotic stability of the conduction solution when all three effects are either destabilizing or stabilizing, are obtained via a symmetrization.     

求解无限域动力刚度矩阵的双渐近算法

采用连分式算法可以有效地求解无限域动力刚度表示的比例边界有限元方程, 它具有收敛范围广、收敛速度快等优点. 该文在高频渐近连分式算法的基础上考虑了低频渐近, 发展了一种针对矢量波动方程的双渐近算法. 随着展开阶数的增加, 双渐近算法可以在全频域范围内快速逼近准确解. 引入了系数矩阵?X(i)来增强连分式算法的数值稳定性. 通过在高频极限、低频极限时满足动力刚度表示的比例边界有限元方程, 建立了递推关系以求得动力刚度矩阵. 通过二维半无限楔形体、三维均质弹性半空间数值算例表明, 双渐近算法比单渐近算法更稳定、优越.     

Stability analysis of plane laminar Poiseuille flow with constant heat flux across the wall: asymptotic methods

Classical linear stability theory is extended to include the effects of temperature and pressure dependent fluid properties. These effects are studied asymptotically by using Taylor series expansions for all properties with respect to temperature and pressure. In this asymptotic approach all effects are well separated from each other, and only the Prandtl number remains as a parameter. In their general form the asymptotic solutions hold for all Newtonian fluids. Two different methods are introduced, a straightforward expansion method and a so called combined method. In the combined method results are found by combining the knowledge of the asymptotic form of the final solution with particular numerical results of the unexpanded basic equations. From the asymptotic results general conclusions can be drawn on how the critical Reynolds number is affected when variable property effects are taken into account.     

Existence and global asymptotic behaviour of positive periodic solution of an SI epidemic model with delays

In this paper, a periodic SI model with delays is studied. By utilizing the Lyapunov–Krasovskii functional method, a novel explicit criterion for the existence and uniqueness and global asymptotic stability of positive periodic solution is established. Finally, a numerical example is given to illustrate the effectiveness of the obtained results.