二阶椭圆型微分方程解的振动定理

考虑二阶非线性椭圆型微分方程∑^n_{i,j}∂/∂x_i{A_{i,j}(x,y)∂/∂x_j}+q(x)f(y)=0 (E)，其中q(x)在外区域 Ω∈R\+n上变号. 利用偏Riccati变换和积分平均技巧, 建立了方程(E)所有解振动的充分准则.     

中学物理教学中的平均值问题

在中学物理教学中,经常用到各种平均值,例如,平均速度、平均作用力、平均功率、平均感生电动势等等.总之,大凡遇到一个变化的物理量,往往就会遇到一个关于它的平均值的问题.但是大多数学生对平均值的理解只停留于n个数的算术平均值上.而在高中物理教学中所接触到的平均值问题几乎全部是"变量的平均",其中包括"变量的算术平均"(如上面提到的各种平均)和"变量的幂平均"(如交流电的有效值即为电流对时间的二次幂平均).并且,无论什么物理量的平均都要考虑是相对于哪一个自变量的平均,而学生对此并没有足够的预备知识,故而在解题过程中的错误层出不穷.本文拟就一道习题的错解重点对此加以说明.     

19F+27Al深部非弹性碰撞产物的角分布

完成了19F+27Al深部非弹性碰撞产物的角分布测量.初步分析了反应产B,C,N,O,F,Ne,Na,Mg和Al的实验室系角分布,展现出深部非弹性反应机制的特点,显示了反应系统随时间的演化过程. Angular distributions of fragments produced in the deep inelastic collision of~(19)F+~(27)Al have been measured for incident energy of 114 MeV at θ_(lab)= 9~(o), 24~(o), 40~(o), 55~(o), 70~(o) and 85~(o). Angular distributions of dissipative products B, C, N, O, F, Ne, Na, Mg and Al are analyzed to provide an evolution process of the intermediate dinuclear system formed in the reaction.     

"受迫振动共振"演示实验的改进

高一物理新教材第九章第七节受迫振动共振中出现了三种频率：物体受迫振动的频率、驱动力的频率和物体的固有频率，对三种频率的理解学生感到困难；其次，对共振曲线的理解也感到很抽象。为此，对本节演示实验进行了较科学的改进，收到了很好的效果。     

碰撞问题浅谈

碰撞是一个重要的物理模型，但同学们对此模型的认识和理解有些困难，下面对此问题进行讨论．     

振动系统的模态分析实验设计

利用模态分析原理和简单试验仪器，得到了直观的悬臂梁和圆盘前4阶模态振型，使学生熟悉了模态分析原理和测试方法，有利于学生对振动规律的理解．     

Effect of Nuclear Binding Energy to K Factor

We modify the square of virtual photon four-momentum by using nuclear binding energy formula, and calculate the effect of nuclear binding energy to K factor and Compton subprocess and annihilate subprocess in A-A collision Drell-Yan process. The outcome indicates that the effect of nuclear binding energy to K factor is obvious in little x region and it would disappear gradually as x increases.     

一类非线性弹簧振子的振动特性分析

设计了一个非线性振动实验装置 ,建立了质点的动力学方程 ,用计算机数值计算并画出运动图、能量图和相图 ,对非线性振动的特点进行了分析     

一类非线性弹簧振子的周期性振动

本文用数值计算的方法讨论了一类非线性弹簧振子的周期性振动及其特点．     

Langevin Simulation of Non-Uniform Granular Gases

We present and study a fractal model of a non-uniform granular system for the first time, based on which wenumerically solve the dynamics actions in the system successfully in one-dimensional case. The multi-mixture is composed of N different particles, whose granularity distribution has the fractal characteristic. The particles are subject to inelastic mutual collisions and obey to Langevin equation between collisions. Far from the equilibrium,i.e. the given typical relaxation time τ of the driving Brownian process is much larger than the mean collision time τc, the results of simulation indicate that the degree of inhomogeneity in the granularity distribution signed by the fractal dimension D of size distribution has great influence on the dynamics actions of the system. The velocity distribution deviates obviously from the Gaussian distribution and the particles cluster more pronouncedly with the larger value of D in the system. The velocity distribution and spatial clnsterization change with D are presented.