含阻尼项二阶泛函差分方程的振动性质

从解的渐近状态入手,应用分类讨论方法和Raccati技巧,讨论了一类广泛的二阶泛函差分方程解的振动性与非振动性,建立了四个新的振动性定理,推广并改进了已有文献中的相关结果.     

高阶线性泛函方程解的振动性

考虑一类高阶线性泛函方程解的振动性,我们获得一些新的振动准则.这些振动准则,推广或改进了一些文献中的某些结果.     

具有负扰动项二阶中立型非线性动力方程的振动性与渐近性质

本文讨论时标上具有负扰动项的二阶中立型非线性动力方程的振动性与渐近性质,获得了适用于所有时标的动力方程解的振动性和渐近性的充分条件,阐述了方程中各项的系数在方程解的定性性质中的作用,推广和改进了已有文献的有关结果,并给出了应用实例.     

高阶混合中立型差分方程的振动性质

研究了一类高阶混合中立型差分方程的振动性质,得到了这类差分方程的振动判据.     

时滞差分方程解的有界性

本文用Ｌｙａｐｕｎｏｖ函数方法研究了时滞差分方程解的有性,我们的结论包含了经典的Ｒａｚｕｍｉｋｈｉｎ有界怀定理作为推论,并避免了在Ｒａｚｕｍｉｋｈｉｎ条件下构造函数Ｐ的困难。     

具有可变时滞的高阶非自治中立型差分方程的振动性

研究具有可变时滞的高阶非自治中立型差分方程△~m(X_n-cx_(n-k)) h(n,x_(n-l_n))=0 (n=0,1,2,...)的振动性．利用Banach空间的压缩映象原理,得到了这类差分方程振动的必要条件．利用偏序集中的Knaster不动点定理,得到了这类方程振动的充分必要条件．同时得到了这类差分方程存在最终正解的准则．     

高阶非线性变时滞差分方程解的渐近性

本文研究了一类高阶非线性变滞量差分方程解的渐近性,给出了该类方程的非振动解当n→＋∞时渐近趋于零或超于某有限非零值的几个充分条件。     

带有分段常数变量的单种群模型的全局稳定性和振动性（英文）

研究了带有分段常数变量的单种群连续模型的全局稳定性和振动性.通过计算将连续模型转化为对应的差分模型,首先研究发现当模型的参数和初值条件满足一定条件时,差分方程的任一正解是单调有界的,且正平衡态是全局渐近稳定的.其次以参数β_1作为分类标准,在两种情况下研究得到当参数r属于某一区间时,差分方程的解是振动的.最后数值模拟验证了理论分析的正确性.     

生物数学学报第18卷2003年总目次

第1期非线性递归差分方程的全局渐近稳定性(英).……,...................……李先义朱德明(1)高阶非线性中立型偏徽分方程解的振动性.......................................……林文赞(8)一般家来二分类性状的贝叶斯连核分析方法...........................……许宗利方积艳(15)两种群相互竟争的SIRS传染病模型的德定性 ..........……,…韩丽涛原三领马知恩(21)兵有年龄结构的按种流行病模型正平衡解的全局德定性.............……,二朱礼营周义仓(27)其Holling第H类功能性反应的播食者一食饵系统的定性分析..……,,...............…     

一阶非线性多时滞微分方程的振动性

考虑一阶非线性多时滞微分方程x′（t）=f（t,x（t-r₁）,x（t-r₂）,…,x（t-r_n））,利用其线性近似方程x′（t）=∑i=1nD_i+1f（t,0,…,0）x（t-r_i）的振动性,给出了方程解振动的一个充分条件,所得结果推广了文献[5]的相关结果.     

Linearized oscillations in population dynamics

A linearized oscillation theorem due to Kulenović, Ladas and Meimaridou (1987,Quart. appl. Math. XLV, 155–164) and an extension of it are applied to obtain the oscillation of solutions of several equations which have appeared in population dynamics. They include the logistic equation with several delays, Nicholson's blowflies model as described by Gurney, Blythe and Nisbet (1980,Nature, Lond. 287, 17–21) and the Lasota-Wazewska model of the red blood cell supply in an animal. We also developed a linearized oscillation result for difference equations and applied it to several equations taken from the biological literature.     

Oscillation frequencies of plant stems with apical loads

The frequency of free oscillations of plant stems with apical loads, as found in some cereals, is different depending on whether the stems are oriented vertically or horizontally. Neglecting the stem's own weight the differential equations describing the oscillation can be solved for both cases, although in the vertical orientation only for a limited set of conditions including constant bending stiffness along the stem. Comparison with experimental data shows that the difference between the oscillation frequencies in vertical and horizontal orientations can be attributed to the fact that in the vertical orientation the top load due to gravity induces a bending moment varying with the oscillation, while in the horizontal case this bending moment is nearly constant.     

一阶泛函差分方程解振动的充分和必要条件

得到具有多个时滞的差分方程：An l-An m^∑i=1piAn-ki=0解振动的充分和必要条件,这里pi全是正数,ki是正整数,i=1,2,3,…,m,(或pi是负数,ki是负整数)。     

非线性高阶阻尼时滞微分方程的振动定理

研究具有阻尼项的非线性时滞微分方程,给出了使得方程的一切解振动的两个充分条件.一些实例说明,本文的结果在判定非线性阻尼方程的振动性时较文献中的结果更为有效.     

Theoretical computation of phase locking in embryonic atrial heart cell aggregates

The effects of periodic stimulation of spontaneously beating aggregates of chick atrial heart cells are considered. Provided the effects of a single stimulus do not change the properties of the oscillation, and that the oscillation is re-established rapidly following a stimulus, this system can be modeled by one-dimensional finite difference equations. These equations employ experimentally generated phase resetting data that describe the effects of a single isolated stimulus at different phases of the oscillation. A complete analysis of the predicted dynamics is given over a broad range of stimulation frequencies and amplitudes. Prominent features of the dynamics include phase locking, bistability, chaos, and disappearance of Arnold tongues at large stimulation amplitudes. The fine details of the bifurcations are sensitive to properties of the phase resetting curves, and consequently, the observed bifurcations are not expected to be "universal" for larger stimulation amplitudes. Experimental traces show many correspondences with theoretical computations.     

Oscillations of plants' stems and their damping: theory and experimentation

Free oscillations of upright plants' stems, or in technical terms slender tapered rods with one end free, can be modelled by considering the equilibrium between bending moments and moments resulting from inertia. For stems with apical loads and negligible mass of the stem and for stems with finite mass but without top loading, analytical solutions of the differential equations with appropriate boundary conditions are available for a finite number of cases. For other cases approximations leading to an upper and a lower estimate of the frequency of oscillation omega can be derived. For the limiting case of omega = 0, the differential equations are identical with Greenhill's equations for the stability against Euler buckling of slender poles. To illustrate, the oscillation frequencies of 25 spruce trees (Picea sitchensis (Bong.) Carr.) were compared with those calculated on the basis of their morphology, their density and their static elasticity modulus. For Arundo donax L. and Cyperus alternifolius L. the observed oscillation frequency was used in turn to calculate the dynamic elasticity modulus, which was compared with that determined in three-point bending. Oscillation damping was observed for A. donax and C. alternifolius for plants' stems with and without leaves or inflorescence. In C. alternifolius the difference can be attributed to the aerodynamic resistance of the leaves, whereas in A. donax structural damping in addition plays a major role.     

Flow in a two-dimensional collapsible channel with rigid inlet and outlet

This paper examines mainly oscillatory behavior of a fluid-conveying collapsible tube using a two-dimensional flexible channel made of a pair of membranes. The equation of equilibrium of the membrane in a large deflection theory is coupled with the equations of continuity and momentum of an incompressible flow in a one-dimensional flow theory accounting for flow separation. An explicit finite difference method was used to solve the governing equations numerically. According to numerical results, the fluids in the inlet and outlet rigid channels have strong effects on the oscillation of the system. Depending on initial values for the numerical integration, there may exist both a stable static equilibrium and an oscillatory solution for the same parameter values, but only if the external pressure is sufficiently large.     

含扩散和时滞的偏微分方程解的振动性

研究一类含扩散和时滞的偏微分方程解的振动性,利用平均法,通过使用偏泛函微分方程上、下解思想和泛函微分方程振动性理论,获得了其解的非负性和关于正平衡态振动的充分条件．     

Zum Mechanismus der biologischen 24-Stunden-Periodik

Summary The level (=arithmetic average of all instantaneous values)of a self-sustained oscillation in general influences all properties of the oscillation, including period, amplitude and shape of the oscillation, and the rate of exchange of energy between the oscillator and its environment. Only when the non-linear damping factor does not depend on the instantaneous value of the oscillating function, but only on the amplitude of the oscillation, are the other properties independent of the average level. The differential equations describing self-sustained oscillations cannot be solved exactly, but methods of approximation are applicable. Numerical solutions to several different forms of the equations will be discussed.In the simplest case (van der Pol equation) all properties of the self-sustained oscillation (e.g. period, amplitude) are extreme when the level is zero. The oscillation continues only within a given range of levels (oscillating range); outside this range, the oscillation damps out. In other modifications of the equation, the oscillating function cannot assume a zero value. In all cases, the extent to which the average level influences the different properties depends on the factor , which describes the position of the oscillation within the range between harmonic and relaxation types of oscillation.In the elementary van der Pol equation, the correlation between level and frequency changes sign within the oscillating range; that is, the circadian rule, demanding an always positive correlation between level and frequency, cannot be fulfilled. Only with an additional non-linearity in the energy of recoil does the correlation remain unchanged in sign throughout the oscillating range. A stability condition demands a positive sign for this non-linearity, and hence, for the correlation (fulfilling the circadian rule); if the sign is negative (violating the circadian rule), the oscillation becomes unstable. With an additional term of the third order, the oscillation acquires a two-peaked shape typical of many circadian oscillations.A simple differential equation describing all general properties of the circadian periodicity must fulfil these conditions: the oscillation must be self-sustained and limited to positive values; and the energy of recoil must be non-linear with a positive coefficient to obtain the appropriate correlation between level and frequency. In the equations here developed the environment directly influences only one parameter of the oscillation, i.e. the level. In addition to the circadian periodicity, the differential equations here examined describe the behavior of several other biological oscillations.

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Die benutzten mathematischen Begriffe folgen — soweit dort angeführt — den Benennungen des DIN-Blattes 1311; im Anhang I sind die wichtigsten Begriffe noch einmal zusammenfassend definiert.