MEMS动平板的切向静电阻力

由于微机械的表面积与体积之比远大于宏机械,所以微机械中的表面阻力难以忽略,为了改善MEMS器件的性能和可靠性,必须对其影响进行研究.基于能量守衡法,本文建立了光滑平板和正方形、四棱锥两种微凸体粗糙表面平板的切向静电阻力模型,讨论了微小尺度、表面形貌、外加电压以及因流片制造工艺而产生的微凸体、凹坑或孔对两个相对运动的带电平板间的切向静电阻力的影响.分析表明：当平板宽度与两平板之间的距离之比、表面形貌因数和外加电压增大时,切向静电阻力也将随之增加;表面形貌因数则与微凸体在平板的总投影面积与平板面积之比成正比,随相对表面粗糙度增加而非线性增加.     

含对称间隙的摩擦振子非线性动力学分析

建立了两自由度含对称间隙的干摩擦碰撞振动系统的动力学模型,分析了系统运动中存在的滑动、黏着及碰撞,分别给出其判断方法和衔接准则,推导出各阶段系统的解析解,并采用数值迭代方法求解和分析了系统的复杂动力学行为,同时分析干摩擦对系统动力学性能的影响.结果表明,系统存在叉式分叉,系统由对称周期运动变为反对称周期运动,进而通过Hopf分叉或周期倍化分叉通向混沌.在参数变化范围较大的情况下,系统存在类型丰富的周期运动、拟周期运动以及混沌;系统存在对称运动、反对称运动对、黏滑碰撞运动以及由初始条件决定的共存吸引子.     

模拟正常刹车条件下C／C复合材料的摩擦表面结构分析

采用MM-1000型摩擦磨损试验机评价粗糙层基体炭C/C复合材料在模拟正常刹车条件下的摩擦磨损性能,借助扫描电子显微镜、微区拉曼光谱仪和红外光谱仪分别研究复合材料摩擦表面的形貌、微区石墨化度及其结构,并通过热失重曲线比较摩擦前后复合材料表面在惰性气氛中的升温失重.结果表明:在模拟正常刹车试验时,C/C复合材料的摩擦系数为0.32,线性磨损量和磨损质量损失分别为0.48 μm和2.12 mg;刹车试验后,摩擦表面由纳米级粒子聚集并压制而成,且摩擦表面炭微晶结构发生变化;在暗灰色的摩擦膜区域,炭微晶的R值从摩擦前的0.207升至1.03,而在白色区域,因炭微晶的接触压力提高而发生应力石墨化,R值降至0.084;摩擦表面能够吸附更多水分,即使在惰性气氛下也比未摩擦表面的升温失重大.     

传动装置密封环摩擦磨损性能研究

为分析车辆传动装置密封环在高速高压工作环境下的磨损失效,利用自主研制的试验台研究了速度、接触压力和介质油温对密封摩擦副摩擦磨损特性的影响;利用扫描电子显微镜观察了磨损程度不同的密封环端面的表面形貌,并探讨了其磨损机理.结果表明,在设定的试验条件下,密封摩擦副的摩擦系数随着压力的增大和转速的升高先急剧减小再降幅减缓后趋于稳定,而压力对摩擦状态的影响要比转速显著.密封环端面温度与摩擦状态之间存在相互影响的特征.密封介质性质同样影响着密封环的摩擦状态.在稳定磨损阶段,密封环的磨损机理以磨粒和黏着磨损为主导,当进入到剧烈磨损期后,磨粒磨损和疲劳磨损的影响更为突出.     

一维六方准晶中带双裂纹的椭圆孔口问题的解析解

利用复变函数方法,通过构造保角映射,研究了一维六方准晶中带双裂纹的椭圆孔口的反平面剪切问题,给出了Ⅲ型裂纹问题的应力强度因子,在极限情形下,不仅可以还原为已有的结果,而且求得一维六方准晶中带双裂纹的圆形孔口问题、十字裂纹问题在裂纹尖端的应力强度因子．     

A Criterion for Stability of Synchronization and Application to Coupled Chua＇s Systems

We investigate synchronization in an array network of nearest-neighbor coupled chaotic oscillators. By using of the Lyapunov stability theory and matrix theory, a criterion for stability of complete synchronization is deduced. Meanwhile, an estimate of the critical coupling strength is obtained to ensure achieving chaos synchronization. As an example application, a model of coupled Chua＇s circuits with linearly bidirectional coupling is studied to verify the validity of the criterion.     

Simulation Study of Shock Reaction on Porous Material

Direct modeling of porous materials under shock is a complex issue. We investigate such a system via the newly developed material-point method. The effects of shock strength and porosity size are the main concerns. For the same porosity, the effects of mean-void-size are checked. It is found that local turbulence mixing and volume dissipation are two important mechanisms for transformation of kinetic energy to heat. When the porosity is very small, the shocked portion may arrive at a dynamical steady state; the voids in the downstream portion reflect back rarefactive waves and result in slight oscillations of mean density and pressure; for the same value of porosity, a larger mean-void-size makes a higher mean temperature. When the porosity becomes large, hydrodynamic quantities vary with time during the whole shock-loading procedure： after the initial stage, the mean density and pressure decrease, but the temperature increases with a higher rate. The distributions of local density, pressure, temperature and particle-velocity are generally non-Gaussian and vary with time. The changing rates depend on the porosity value, mean-void-size and shock strength. The stronger the loaded shock, the stronger the porosity effects. This work provides a supplement to experiments for the very quick procedures and reveals more fundamental mechanisms in energy and momentum transportation.     

Approximation of thermoelasticity contact problem with nonmonotone friction

The paper presents the formulation and approximation of a static thermoelasticity problem that describes bilateral frictional contact between a deformable body and a rigid foundation. The friction is in the form of a nonmonotone and multivalued law. The coupling effect of the problem is neglected. Therefore, the thermic part of the problem is considered independently on the elasticity problem. For the displacement vector, we formulate one substationary problem for a non-convex, locally Lipschitz continuous functional representing the total potential energy of the body. All problems formulated in the paper are approximated with the finite element method.