水平随机地震激励下弹性圆拱的半解析法

结合虚拟激励法与Galerkin法,研究弹性圆拱在水平随机地震作用下随机响应的半解析解.在建立圆拱平面内动力平衡微分方程的基础上,通过选取适当的试函数,应用Galerkin法将动力平衡微分方程转化为线性常微分方程组.通过设定虚拟荷载,采用确定性方法求解响应量的功率谱密度函数的近似解,得到圆拱随机振动问题的闭合解.该方法无须计算拱的振型,对非正交阻尼同样适用.通过算例分析和与有限元计算结果的比较,验证了该方法的计算精度.当采用的试函数与圆拱振型接近时,采用较少的试函数就能获得较高的精度,该方法是一种简便、高效的方法.     

振动式排种器的模态分析与试验研究

针对有限元分析中排种器中铰链建模的困难,提出用杆单元模拟铰接点运动和动力学特性的近似处理方法,建立了排种器的整体模型,分析了系统的前四阶固有频率和对应的振型图。模态试验结果与仿真分析结果对比表明,所建立的有限元计算模型是准确的。根据分析结果及排种器的工作特点,其工作频率为4 Hz左右。     

装甲车噪声源诊断

文章通过实验及其信号处理得到了各轮子的声力传递函数。根据这些测量与分析结论可以定量比较装甲车四种轮子受到同样大小的力激励时,其振动和声辐射通过各传递环节而对车内声场的综合贡献大小。以便在降低装甲车车内噪声时,确定哪种轮子是应该着重考虑采取降噪措施的对象,为装甲车降噪措施的合理化研究提供一定的科学依据。     

GD2308高速加固缝纫机压脚有限元建模与分析

以工业缝纫机的减振降噪为应用背景,针对其结构特点及工作特性,通过CATIA对GD2308高速加固缝纫机压脚进行有限元建模,应用有限元软件ANSYS对压脚进行网格的划分,生成有限元分析模型,对压脚进行动态特性分析,计算压脚的前10阶固有频率与前6阶振型,给出振型图.分析结果表明,压脚结构振动主要表现为弯曲、扭转和弯扭组合...     

车辆-轨道-桥梁空间耦合振动引起的环境振动

首先建立了车辆-无碴轨道-桥梁系统空间耦合振动模型,通过随机振动分析得到桥墩墩底反力,然后建立了土体-建筑物的三维有限元模型,并将以上得到的墩底反力作为土体-建筑物三维有限元模型的外部激励。分析结果表明,周围土体振动强度随距离的增加而减小,且都存在反弹区 周围建筑物的振动强度随桥墩距离的增大而减小,且在建筑物低层横向和竖向振动相差不大,但是到了高层处横向振动明显大于竖向振动。     

Extrusion of ultrahigh molecular weight polyethylene under ultrasonic vibration field

The effects of polypropylene (PP) and ultrasonic irradiation on the processing and mechanical properties of ultrahigh molecular weight polyethylene (UHMWPE) are studied. The results show that PP can effectively improve the fluidity and mechanical properties of UHMWPE. The Izod notched impact strength increases from 92 kJ/m² for pure UHMWPE to 109.2 kJ/m² for the blend of UHMWPE with 10 wt % PP. The Young's modulus increases from 528 MPa for pure UHMWPE to 1128 MPa when 25 wt % PP is contained in the blend, and the yield strength also rises when PP is added. The application of ultrasonic vibrations during extrusion can prominently decrease the die pressure and apparent viscosity of the melt, thus increasing the output of extrudate. An appropriate ultrasonic intensity and irradiation time can further promote the mechanical properties, while an overdose of irradiation destroys them. © 2003 Wiley Periodicals, Inc. J Appl Polym Sci 89: 2628–2632, 2003     

Homogeneous Fluidization Characteristics of Vibrating Fluidized Beds

The effects of vibration parameters, operating conditions and material properties on fluidization quality were investigated by the measurement and analysis of voidage fluctuation signals in a vibrating fluidized bed with a diameter of 148 mm. The fluctuation deviation of the bed voidage and the enhancement index of the bed derived can describe bed homogeneity and its extension. A new criterion of homogeneity, consisting of the material parameter (Ar), operating parameters (H₀, u/u_mf) and vibration parameters (a, ω), is proposed to predict a suitable range of homogeneous fluidization. Experimental results on eight kinds of solids, five static bed heights and different vibration parameters were used to propose guidelines for the reasonable selection of operating conditions for vibrating fluidization and better operating conditions.     

基于循环维纳滤波的振动信号去噪算法研究

振动信号的去噪需要在滤除噪声的同时尽可能避免相位失真。传统的锐截止低通滤波器或FIR滤波器无法在去噪效果和线性相位之间取得平衡,难以满足振动信号的去噪需求。针对这一问题,将线性相位的维纳滤波算法引入到振动信号的去噪中,并结合振动信号的循环平稳特性,形成了振动信号的循环维纳滤波算法。文中以直接维纳滤波为基础对循环维纳滤波算法的原理进行了深入分析和仿真实现,并基于实测汽轮机振动信号对算法的去噪性能进行了讨论。理论分析及算法仿真表明,循环维纳滤波算法在保证线性相位的前提下有较好的去噪效果,能够解决传统去噪算法所存在的去噪效果与线性相位难以均衡的问题。     

CJ91胶粘剂在螺旋振动光整机中的应用

螺旋振动光整机槽内壁的橡皮保护层由于老化及磨损等原因出现裂口甚至脱落现象，严重影响设备的使用寿命和闸把壳体的外观质量。通过分析和试验筛选出螺旋振动光整机的理想胶粘荆——CJ91胶粘剂并介绍了粘接修补工艺。     

Mathematical model of shear rate of polymer melt dynamic extruding through capillary

With superimposing a sine vibration of displacement on the extruding direction of a polymer melt, the characterization formula of the shear rate of a polymer melt within a capillary was set up. By making use of the experimental equipment of a constant velocity type dynamic rheometer of capillary (CVDRC) designed by the authors, the calculating steps of the shear rate of the polymer melt at the wall of the capillary under a vibration force field were established. Through measuring and analyzing the instantaneous data of capillary entry pressure, capillary volume rate, and their phase‐difference under the superimposed vibration, the polymer melt's shear rate at the wall of the capillary can thus be calculated. © 2005 Wiley Periodicals, Inc. J Appl Polym Sci 95: 1056–1061, 2005