Lienard方程的比较原理

证明了几个比较原理,使方程x〃+f(x)x'+g(x)=0的周期解的存在性与解的有界性定理可以分别用来判定方程x"+h(x,x')x'+g(x)=0的周期解的存在性与解的有界性.     

含有各阶导数的四阶两点边值问题正解的存在性

利用一个新的锥不动点定理,研究含有各阶导数四阶两点边值问题{x~((4))(t)+Ax'(t)=λf(t,x(t),x'(t),x'(t),x''(t)),0t1 x(0)=x(1)=x'(0)=x'(1)=0正解的存在性.其中f是一个非负连续函数,λ0,0Aπ~2.     

自适应迎风格式求解奇异摄动两点边值问题的高精度算法(二)

0引言 考虑与文[1]相同的奇异摄动两点边值问题的数值解法: Tu(x):=-εu″(x)-p(x)u′(x)=f(x),x∈(0,1); (1) u(0)=0,u(1)=1. (2) 其中ε是一个常数,0<ε≤1,f∈C2[0,1].假定P∈C3[0,1]且存在常数β和-β使得0<β≤p(x)≤-β,|p′(x)|≤-β,(V)x∈[0,1] (3) 成立.     

Liénard方程的比较原理

本文证明了一个比较原理，使方程x" f(x)x' g(x)=0的周期解存在性定理可以用来判断方程x" h(x，x')x' g(x)=0的周期解的存在性．     

具p-Laplacian算子型奇异方程组边值问题正解的存在性

本文讨论了一类具p-Laplacian算子型奇导方程组边值问题(φp(x'))'+α1(t),f(x(t),y(t))=0,(φp(y'))'+α2(t)g(x(t),y(t))=0,x(0)-β1x'(0)=0,x(1)+δ1x'(1)=0,y(0)-β2Y'(0)=0,y(1)+δ2y'(1)=0正解的存在性,其中φp(x)=|x|p-2x,p>1.通过使用不动点指数定理,在适当的条件下,建立了这类奇异方程组边值问题存在一个或者多个正解的充分条件.这些结果能用来研究椭圆型方程组边值问题径向对称解的存在性.     

Volterra型积分微分方程奇摄动边值问题

本文首先研究积分微分方程x″=f(t,X,x′,Tx)满足边界条件x(0)=A,x(1)=B的边值问题,其中[Tx](t)=φ(t)+integral from 0 to t K(t,s)x(s)ds,K(t,s)≥0于[0,1]×[0,1]上连续,φ(t)于[0,1]上连续,证明解的存在定理,然后研究奇摄动积分微分方程εx″=f(t,X,X′,Tx,ε)＇满足同类边界条件的边值问题,其中ε>0是小参数。我们利用构造上下解的方法,证明解的存在定理,给出解的估计。     

三阶非线性边值问题的奇摄动(英)

本文利用Volterra型积分算子和微分不等式技巧给出了一类三阶非线性微分方程奇摄动边值问题：εX＝f（t，x，x，ε，x（0）＝A，g（x'（0），（0），ε）＝0，h（x（1），x（1），ε）＝0解的存在性．唯一性及渐近估计．     

拟线性常微分方程组边值问题解的估计

本文研究拟线性常微分方程组边值问题x′=f(t,x,y,ε),x(0,ε)=A(ε) εy″=g(t,x,y,ε)y′+h(t,x,y,ε) y(0,ε)=B(ε),y(1,ε)=C(ε)的奇摄动。其中x,f,y,h,A,B和C均属于Rn,g是n×n矩阵函数。在适当的条件下,利用对角化技巧和不动点定理证明解的存在,并估计了余项.     

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.     

具共振条件下的一类三阶非局部边值问题的可解性

本文考虑一类三阶非局部边值问题x”’(t)=f(t,x(t),x'(t),x”(t)),t∈(0,1), x(0)=0,x'(0)=0,x'(1)=(?) x'(s)dg(s),其中f:[0,1]×R3→R是一个连续函数, g:[0,1]→[0,∞)是一个非减的函数,且满足g(0)=0．在g满足共振条件g(1)=1 的情况下,通过应用重合度理论,得到了该问题解的存在性结果．     

Expansions of Dirichlet to Neumann operators under perturbations

We obtain an asymptotic expansion of the Dirichlet to Neumann operator (DNO) for the Dirichlet problem on perturbations of the unit disk. We write our result in terms of pseudodifferential operators which themselves have expansions in the perturbation parameter. For a given power of the perturbation parameter, m > 0, and a given order, n < 0, we give an algorithm which allows for the expansion of the symbol of the DNO up to mth power in the perturbation parameter, with error terms belonging to symbols of order n.     

Pseudopower expansion of solutions of generalized equations and constrained optimization problems

We show that the solution of a strongly regular generalized equation subject to a scalar perturbation expands in pseudopower series in terms of the perturbation parameter, i.e., the expansion of orderk is the solution of generalized equations expanded to orderk and thus depends itself on the perturbation parameter. In the polyhedral case, this expansion reduces to a usual Taylor expansion. These results are applied to the problem of regular perturbation in constrained optimization. We show that, if the strong regularity condition is satisfied, the property of quadratic growth holds and, at least locally, the solutions of the optimization problem and of the associated optimality system coincide. If, in addition the number of inequality constraints is finite, the solution and the Lagrange multiplier can be expanded in Taylor series. If the data are analytic, the solution and the multiplier are analytic functions of the perturbation parameter.     

两参数非线性反应扩散积分微分方程的内层激波渐近解

研究了一类两参数非线性反应扩散积分微分奇摄动问题.利用奇摄动方法,构造了问题的外部解、内部激波层、边界层及初始层校正项,由此得到了问题解的形式渐近展开式.最后利用积分微分方程的比较定理证明了该问题解的渐近展开式的一致有效性.     

Singular perturbation analysis of a certain volterra integral equation

An investigation is made of the asymptotic behavior of the solutionu(t;ε) to the Volterra integral equation $$\varepsilon u(t;\varepsilon ) = \pi ^{ - \tfrac{1}{2}} \int\limits_0^t {(t - s)^{ - \tfrac{1}{2}} [f(s) - u^n (s;\varepsilon )]} ds, t \geqslant 0, n \geqslant 1$$ , in the limit as ε→0. This investigation involves a singular perturbation analysis. For the linear problem (n=1) an infinite, uniformly valid asymptotic expansion ofu(t;ε) is obtained. For the nonlinear problem (n≥2), the leading two terms of a uniformly valid expansion are found     

无胀缝坡道路面板热胀屈曲的摄动解

文中分析了无胀缝坡道路面板在温度场作用下热胀屈曲的力学机制.采用正则摄动法导出了坡道路面板临界铺设温差的渐近表达式,分析了坡道与水平直道路面板临界铺设温差之间的关系,得出了坡道与水平直道路面板热胀屈曲的统一解答,并据此给出了无胀缝坡道路面的合理铺设温差.     

A NUMERICAL PERTURBATION EXPANSION METHOD FOR THE SOLUTION OF A LIENARD-TYPE INITIAL-VALUE PROBLEM WITH PERIODIC DECAYING FORCING TERM

A numerical perturbation expansion method is developed, analysed and implemented for the numerical solution of a second-order initial-value problem. The differential equation in this problem exhibits cubic damping, a cubic restoring force and a decaying forcing-term which is periodic with constant frequency. The method is compared with the numerical method by Twizell [1]. In fact, the later is first perturbation approximate solution in the present paper.     

Analyzing the longitudinal effect of hypersonic flow past a conical cone via the perturbation method

To analyze the hypersonic flow past a conical cone, the variations of gasdynamic properties subjected to the longitudinal curvature effect by using the perturbation method. An outer perturbation expansion has been carried out by recent researchers, but a problem occurred, the outer expansion solutions are not uniformly valid in the shock layer, however, the outcome near the conical body surface called vortical layer remains deflective. This study intends to discover uniformly valid analytical solutions in the shock layer by applying the inner perturbation expansions matching with the out expansions to analyze the characteristics in the whole region including shock layer and vortical layer. Starting from the zero-order approximate solutions for hypersonic conical flow is then applied as the basic solutions for the outer perturbation expansions of a flow field. The governing equations and boundary conditions are also expanded via outer perturbations. Using an approximate analytical scheme in the derivation process, first-order perturbation equations can be simplified and the approximate closed-form solutions are obtained; furthermore, the various flow field quantities, including the normal force coefficient on the cone surface, have been calculated. According to the variations of gasdynamic properties, the longitudinal curvature effect for the hypersonic flow past a conical cone can be determined. Thicknesses of shock layer and vortical layer can be predicted as well. The physical phenomena inside both layers can be investigated carefully, the conditions for an elliptic cone with longitudinal curvature, m = 1 and n = 2 and other conditions of parameters; the perturbation parameter, ε_m2 = 0.1, semi-vertex angle of the unperturbed cone, δ = 10°, and hypersonic similarity parameter, K_δ = M_∞δ = 1.0, the thickness of vortical layer, η_VL, can be calculated at the position angle of conical cone body, ? = 30° was demonstrated here. Results show how very thin the vortical layer is approximately only 10% of the shock layer close to the body, the pressure in the whole shock layer is verified to be uniformly valid which agrees with previous studies. Large gradient changes in entropy and density are found when the flow approaches the cone surface, the most important is, this method provides a benchmark solution to the hypersonic flow past a conical cone and to assist the grids and numerics for numerical computation should be fashioned to accommodate the whole flow field region including the vortical layer of rapid adjustment, and let the analysis become more effective and low cost.     

Asymptotic decay of solutions of the liouville equation under perturbations

We consider the Cauchy problem for a perturbed Liouville equation. An asymptotic solution is constructed with respect to the perturbation parameter by the two-scale expansion method; this construction can be applied over long time intervals. The main result is the definition of a deformation of the leading term of the asymptotic expansion within a slow time scale. Translated frommatematicheskie Zametki, Vol. 68, No. 2, pp. 195–209, August, 2000.     

Perturbation of the q-numerical radius of a weighted shift operator

We formulate the Taylor series expansion for the q-numerical radius of a weighted shift operator with periodic weights near q=0. Coefficients up to the fourth order in the expansion are found via the perturbation theory of Hermitian matrices.     

关于耦合型对流-扩散方程组的奇异摄动边值问题

本文考虑下述耦合型对流-扩散方程组的奇异摄动边值问题:本文提出两种方法:一种是初值化解法,用这种方法,原始问题转化成一系列没有扰动的一阶微分方程或方程组的初值问题,从而得到一个渐近展开式;第二种是边值化解法,用这种方法,原始问题转化成一组没有边界层现象的边值问题,从而可以得到精确解和使用经典的数值方法去得到具有关于摄动参数ε一致的高精度数值解.