圆截面弹性细杆的平面振动

基于Kirchhoff理论讨论圆截面弹性细杆的平面振动．以杆中心线的Frenet坐标系为参考系建立动力学方程．杆作平面运动时,其扭转振动与弯曲振动解耦．讨论任意形状杆的扭转振动和轴向受压直杆在无扭转条件下的弯曲振动,证明直杆平衡的静态Lyapunov稳定性与欧拉稳定性条件为动态稳定性的必要条件．考虑轴向力和截面转动惯性效应的影响,导出弯曲振动的固有频率．     

复弯矩表示的非圆截面杆平衡的Schrǒdinger方程及其半解析解

弹性细杆的平衡和稳定性问题的研究在工程和分子生物学中有重要的应用背景。利用文中提出的复柔度概念，建立了用复弯矩表示的非圆截面杆平衡的Schrǒdinger方程。借助复曲率概念，导出以杆的曲率、挠率和截面相对Frenet坐标系的扭角为未知变量的2阶常微分方程，此方程与传统使用的Kirchhoff方程等价。文献中仅适用于圆截面杆平衡问题的Schrǒdinger方程为本文导出方程的特例。对于准对称截面杆，用小参数法分别建立了零次和一次近似方程，其中零次近似方程存在解析解。对于截面的主轴坐标轴与中心线的Frenet坐标轴重合的无扭转杆特殊情形，Schrǒdinger方程转化为Duffing方程，应用数值方法作出了Duffing杆变形后的三维几何图形。     

非圆截面弹性细杆的螺旋线平衡及稳定性

本文研究端部受力和力矩作用，且存在初曲率和初扭率的非圆截面弹性细杆的螺旋线平衡及其稳定性。描述弹性细杆平衡状态的Kirchhoff方程存在与杆的螺旋线平衡状态相对应的特解。直杆和圆环杆为螺旋线状态的两种特例。文中分析了螺旋线的几何特性与作用力和力矩之间的相互关系，并导出螺旋线平衡的一次近似解析形式稳定性判据。分析表明，松弛状态下弹性杆可处于螺旋线状态，直杆只有在轴向压力的作用下才能保持螺旋线平衡。无初曲率和初扭率弹性杆的螺旋线平衡稳定性必要条件是杆截面绕副法线轴的抗弯刚度大于或等于绕法线轴的抗弯刚度。此条件也适用于带初扭率的圆环杆及更普遍情形。无初曲率和初扭率的圆截面杆的螺旋线平衡恒稳定。     

复弯矩表示的非圆截面杆平衡的Schrdinger方程及其半解析解

弹性细杆的平衡和稳定性问题的研究在工程和分子生物学中有重要的应用背景。利用文中提出的复柔度概念,建立了用复弯矩表示的非圆截面杆平衡的Schrdinger方程。借助复曲率概念,导出以杆的曲率、挠率和截面相对Frenet坐标系的扭角为未知变量的2阶常微分方程,此方程与传统使用的Kirchhoff方程等价。文献中仅适用于圆截面杆平衡问题的Schrdinger方程为本文导出方程的特例。对于准对称截面杆,用小参数法分别建立了零次和一次近似方程,其中零次近似方程存在解析解。对于截面的主轴坐标轴与中心线的Frenet坐标轴重合的无扭转杆特殊情形,Schrdinger方程转化为Duffing方程,应用数值方法作出了Duffing杆变形后的三维几何图形。     

轴向受压螺旋杆的平衡稳定性

在Kirchhoff动力学比拟基础上讨论端部受轴向压力作用的圆截面弹性细杆的螺旋线平衡稳定性问题.弹性杆的平衡状态由Euler角描述的弹性杆平衡方程的特解确定.从Lyapunov或Euler的不同稳定性概念出发,对弹性杆的平衡稳定性的判断可得出不同的结果.根据一次近似扰动方程判断,弹性杆的螺旋线状态和圆环状态恒满足Lyapunov稳定性条件.但螺旋杆在轴向压力到达临界值时,圆环杆在扭转数到达临界值时将产生屈曲而丧失Euler稳定性.导出临界载荷和临界扭转数的计算公式.螺旋杆的临界载荷取决于螺旋线的高度和螺旋角.螺旋角趋近于π/2时螺旋杆转化为带扭率的直杆,其临界载荷的极限值与压杆的Euler载荷一致.文中对两类不同稳定性概念的区别和联系作出解释.     

Kovalevskaya弹性杆

应用Kirchhoff比拟讨论Kovalevskaya情况弹性细杆的平衡稳定性问题．导出Kirchhoff方程的解析积分．对于杆截面的主轴与Frenet坐标轴重合的无扭转杆的特殊情形作定性分析，讨论其平衡状态的稳定性与分岔．证明了判断受拉扭作用的圆截面直杆平衡稳定性的Greenhill公式也适用于Kovalevskaya情形的非圆截面杆．     

开闭裂纹转子的弯扭耦合振动研究

以水平放置的Jeffcott裂纹转子为研究对象,建立了开闭裂纹转子弯扭耦合振动的非线性运动微分方程,并用数值方法分析了纯弯曲振动与弯扭耦合振动情况下转子的动力响应.结果表明:弯扭耦合振动是由转子质量的偏心和转子自重的共同作用而产生的,当质量偏心很小时可以不考虑扭转振动的影响.当偏心较大时,扭转对弯曲振动的影响主要体现在高转速部分,且由于裂纹开闭的作用,使扭转的耦合作用存在一个范围.随裂纹深度的增加,扭振影响的转速下限就会越低,但当裂纹较深、转速较快时,扭转对弯曲振动在作用范围内有明显的影响,使频谱图和轴心轨迹都发生较大的变化,且对转速的变化极为敏感.因此在故障诊断时必须对扭转的耦合作用高度重视.     

轴向受压螺旋杆的动态稳定性与振动

基于Kirchhoff理论讨论端部受轴向压力作用的圆截面弹性螺旋杆的动态稳定性问题。以杆中心线的Frenet坐标系为参考系,建立用欧拉角描述的弹性杆动力学方程。杆的螺旋线平衡状态由方程的特解确定。基于静力学分析的结论,在动力学范畴内继续讨论轴向受压螺旋杆平衡状态的稳定性。在一次近似意义下证明了螺旋杆在空间域内的欧拉稳定性条件为时域内的Lyapunov稳定性条件。从而进一步认识Lyapunov和欧拉两种不同稳定性概念之间的相互关系。导出轴向受压螺旋杆弯扭耦合振动固有频率的近似解析表达式。     

高频扭转振动对钻井过程破岩特性的影响研究

为了研究高频扭转振动钻井对PDC(Polycrystalline Diamond Compact)钻头破岩的影响,基于弹塑性力学和机械振动原理,分别建立切削齿的切削模型和岩石的振动方程,并指出了岩石的响应特点。通过岩石的应力-应变试验,得到了岩石的等效塑性应变率与岩石剥落之间的关系。依据现场试验与分析计算,研究了高频扭转振动频率对钻井机械钻速的影响。研究结果表明:当钻井扭振频率为岩石的共振频率时,岩石的塑性应变率为1.5%,钻井的机械钻速为6.3mm/s。研究方法与结论对于利用高频扭振提高破岩效率研究具有重要的应用意义。     

极坐标系下扇形截面杆扭转问题的有限差分法

导出了极坐标系下扇形截面杆扭转问题的差分格式；结合Mathcad编程用逐次超松弛迭代法求出了扭转应力函数差分值；采用复化二维辛普生求积公式计算了抗扭刚度；求出了相应的扭转应力的差分解；给出了张角为2π时裂纹尖端附近的第三型应力强度因子．     

Meshless methods for the inverse problem related to the determination of elastoplastic properties from the torsional experiment

The problem of determining the elastoplastic properties of a prismatic bar from the given experimental relation between the torsional moment M and the angle of twist per unit length of the rod’s length θ is investigated as an inverse problem. The proposed method to solve the inverse problem is based on the solution of some sequences of the direct problem by applying the Levenberg-Marquardt iteration method. In the direct problem, these properties are known, and the torsional moment is calculated as a function of the angle of twist from the solution of a non-linear boundary value problem. This non-linear problem results from the Saint-Venant displacement assumption, the Ramberg–Osgood constitutive equation, and the deformation theory of plasticity for the stress–strain relation. To solve the direct problem in each iteration step, the Kansa method is used for the circular cross section of the rod, or the method of fundamental solutions (MFS) and the method of particular solutions (MPS) are used for the prismatic cross section of the rod. The non-linear torsion problem in the plastic region is solved using the Picard iteration.     

Stability and vibration of a helical rod constrained by a cylinder

The stability and vibration of an elastic rod with a circular cross section under the constraint of a cylinder is discussed. The differential equations of dynamics of the constrained rod are established with Euler’s angles as variables describing the attitude of the cross section. The existence conditions of helical equilibrium under constraint are discussed as a special configuration of the rod. The stability of the helical equilibrium is discussed in the realms of statics and dynamics, respectively. Necessary conditions for the stability of helical rod are derived in space domain and time domain, and the difference and relationship between Lyapunov’s and Euler’s stability concepts are discussed. The free frequency of flexural vibration of the helical rod with cylinder constraint is obtained in analytical form. The project supported by the National Natural Science Foundation of China (10472067). The English text was polished by Yunming Chen.     

大变形轴向运动梁的精确动力学模型

轴向运动梁的横向振动是具有实际工程背景的动力学问题.该文应用Cosserat弹性杆模型讨论圆截面轴向运动梁的动力学建模及其运动稳定性.以沿梁中心线的弧坐标代替方向固定的坐标轴,根据梁截面的姿态随弧坐标和时间的变化确定梁的变形过程.从欧拉的速度场概念出发,考虑梁截面转动的惯性效应和剪切变形,建立大变形轴向运动梁的动力学方程.其小变形特例为轴向运动的三维Timoshenko梁.基于该模型分析了轴向运动梁准稳态运动的静态和动态稳定性,导出可导致失稳的临界轴向速度.证明空间域内的欧拉稳定性条件是时间域内的Lyapunov稳定性的必要条件.      

Equations of oscillations of rods of variable composition

We obtain differential equations for the general case of longitudinal, torsional, and transverse oscillations of rods to some parts of which masses are being added or detached. We solve certain special problems concerning the oscillations of such rods of variable composition. In deriving generalized equations of oscillations of rods of variable composition we employ the assumption of planar sections, the assumption of small deformations, and other customary simplifications. We also employ the simplifying assumption of close action; i.e., we assume that the masses being detached and added interact with the rod only at the instant of direct contact. Forces of internal nonelastic resistance are not taken into account. We assume also that in the undeformed state the elastic axis is rectilinear and that the centers of gravity of cross sections are not displaced from their initial positions relative to the cross sections. There may be a change of mass per unit length of the rod both on account of a change in density as well as on account of a change in area of a cross section, the latter being understood to be the union of the initial area of the cross section and the areas of the parts being added and detached. In addition, with the rod there may be associated particles of variable mass distributed continuously or discretely along the length of the rod. We assume that these particles do not interact among themselves but only with the rod.Translated from Zhurnal Prikladnoi Mekhaniki i Tekhnicheskoi Fiziki, No. 1, pp. 103–108, January–February, 1972.     

Compensation of torsion in rods by piezoelectric actuation

This paper considers the compensation of torsional deformations in rods with the help of thin integrated piezoelectric actuator layers. A laminated orthotropic rod is considered, for which the material properties of each layer are assumed to be homogenous. For the sake of a generalization, the piezoelectric actuation is expressed in terms of eigenstrains. The main scope is the derivation of a distribution of eigenstrains that is able to completely compensate the angle of twist caused by external torsional moments. Saint Venant’s theory of torsion for laminated orthotropic rods is extended for the presence of eigenstrains, which is performed by introducing an additional warping function. It is shown that the actuating torsional moment is a function of the eigenstrains and the additional warping function. For the example of a rectangular cross section, an analytic solution for the actuating moment and the additional warping function is presented. The results are verified by three-dimensional finite-element computations showing a very good accordance with the theoretical results over a large parameter range.     

受圆柱面约束弹性杆的平衡与稳定性

讨论受圆柱面约束的圆截面弹性杆的平衡与稳定性。以描述截面姿态的欧拉角为变量,建立受约束弹性杆的平衡方程。利用方程的初积分导出约束力、截面内力及挠性线的解析表达式。作为特殊的平衡状态,讨论杆的螺旋线平衡的存在条件。用相平面法分析螺旋线平衡的稳定性,导出解析形式的稳定性条件。