迷宫密封双控制体模型的改进及应用

由双控制体模型的三个控制方程入手,将其无量纲化,并分解为零阶和一阶无量纲方程.由零阶方程求得定常流场,继而求解一阶方程得到密封的动特性参数,其中一阶方程以简洁的矩阵形式表达,操作更为简便.本文双控制体模型是较为成熟且得到认可的分析方法,双控制体改进模型具有更为清晰的模型及更为简洁的算法.最后与传统模型计算结果比较,验证了本文算法的准确性.随后分析了几种密封参数对其动力特性的影响,揭示某些规律并给出一些建议.     

大间隙环流壁面摩擦及偏心转子静特性研究

基于紊流整体流动模型和Ｍｏｏｄｙ壁面摩擦系数方程简化了大间隙环流三维流非线性偏微分控制方程组,推导了零阶摄动方程并采用数值方法对大间环流中偏心转子静特性进行了深入研究。实例计算结果表明：大间隙环流中转子与以灿承和密封为代表的小间隙环流中转子的静特性有很大同;壁面摩擦系数沿周向变化,同时转子和静子壁面粗糙度以及偏心率对大间隙环流中转子静特性有较大的影响。     

蜂窝密封内流动传热及转子动力特性的研究进展

蜂窝密封由于其具有优良的密封性能和转子动力特性而广泛应用于叶轮机械中.本文从实验研究、数值模拟和理论分析3个方面对蜂窝密封的研究现状及其进展进行了综述.主要内容包括:蜂窝密封泄漏特性及其密封机理的研究进展;蜂窝密封流动总温升特性的研究进展;蜂窝密封流热耦合作用下的流动传热特性研究进展;蜂窝密封非定常气流激振和转子动力特性的流固耦合机理研究进展.最后在蜂窝密封研究现状综述的基础上, 展望了蜂窝密封的发展方向.      

迷宫密封中流场的有限差分模拟

本文用k-ε紊流模型和可压缩流体压力修正方程以及SIMPLEC算法对时均形式的二维N-S方程进行了求解,得到了单腔室迷宫密封中的流场特性,其结果可以用来改进迷宫密封转子动力特性的分析模型.     

涡轮泵转子-迷宫密封系统的非线性稳定性和分岔

研究迷宫密封对某一工程涡轮泵转子系统动力特性的影响,迷宫密封力采用Muszynska非线性力模型,应用有限元法建立转子系统的动力学方程,采取系统动力学方程中包含的高阶线性自由度和低阶的非线性自由度进行分块处理的方法,有效地缩短了求解时间。根据Floquet理论,判别系统的临界失稳转速,并由Floquet乘子来确定系统失稳后分岔方式。采用分块-Newmark法数值模拟了转子二涡轮盘的轴心轨迹。最后分析了涡轮泵转子二涡轮盘的质量偏心同相位和存在90度相位差时对转子系统运动特性的影响。     

迷宫密封转子系统非线性动力稳定性的研究

研究迷宫密封对转子系统动力稳定性的影响，迷宫密封的气动力采用Muszynska非线性力模型，计算了单盘Jeffcott转子非线性动力学特性。对Jacobi矩阵的分析表明，在密封力的影响下，转子达到一定转速后开始失稳，发生Hopf分岔，进入周期涡动状态，涡动幅度随转速的提高而增大，提高到一定程度，密封和转子发生碰摩，采用Runge-Kutta法数值模拟了转子的轴心轨迹。最后分析了迷宫密封的物理和结构参数对系统运动特性的影响。     

大间隙环流中偏心转子动特性系数的数值分析方法

基于作者用整体流动理论和Moody壁面摩擦系数方程建立的大间隙环流中转子动特性系数数值计算模型,应用摄动方法推导了大间隙环流流场非线性控制方程组的一阶摄动方程,提出了求解大间隙环流中偏心转子动力学特性系数的数值分析方法。用该方法得到的数值结果与已有的解析解和实验结果具有较好的一致性。     

具有封严蓖齿转子系统的动力稳定性分析

封严蓖齿的气弹力对转子系统的稳定性起重要作用，本文建立了具有封严蓖齿的转子系统动力稳定性的分析方法，该方法利用传递矩阵法建立系统的主导方程，将封严蓖齿的气弹力以等效刚度及等效阻尼系数的方式引入转子系统的主导方程，用数值积分法解主导方程，求得系统的动力特性，根据扰动解判断系统的稳定性。本文所建立的分析软件，也可计算转子系统的不平衡响应、临界转速、突加不平衡响应等。文中对一模型转子进行了算例分析。     

随机结构动力特性分析格林函数法

在考虑材料参数和几何参数小变异情况下,采用一阶近似方法将随机杆件动力特性分析的控制微分方程分解为关于动力特性均量和偏量的两组控制微分方程,然后利用这两组方程在形式上与静力问题控制微分方程的相似性,采用静力问题基本解以及域外布设虚荷载方法和多域耦合技术,提出了随机结构动力特性分析格林函数法.从数值算例可以看出,在小变异情况下,本文方法的结果与Monte-Carlo法的结果相当吻合,计算精度较高;在计算效率方面,本文方法的计算量远少于摄动随机有限元法的计算量.     

带尾翼水下自然超空泡射弹数值模拟研究

基于Navier-Stokes方程,考虑气液间相变,采用大涡模拟湍流模型,PISO算法及VOF方法,利用自行开发的程序对绕三维带尾翼水下自然超空泡射弹的非定常空泡流动进行了数值模拟研究.通过计算结果得到超空泡从射弹头部初生至完全包裹弹身的形成过程.在此基础上,计算不同攻角条件下的超空泡形态,并给出射弹表面空泡厚度分布曲线,分析不同攻角对超空泡形态特性的影响规律,以及在零攻角条件下,分析尾翼对空泡形态的影响.另外计算不同空化数条件下的超空泡无量纲长度和厚度,将计算结果与实验数据进行对比,两者吻合较好.研究结果为进一步研究水下高速射弹的水动力特性和弹道特性问题提供理论基础.     

The 7th International Conference on Fluid Mechanics May 24-27,2015,Qingdao,China

正http://www.icfm7.org First Announcement and Call for PapersThe objective of International Conference on Fluid Mechanics(ICFM)is to provide a forum for researchers to exchange new ideas and recent advances in the fields of theoretical,experimental,computational Fluid Mechanics as well as interdisciplinary subjects.It was successfully convened by the Chinese Society of Theoretical and Applied Mechanics(CSTAM)in Beijing(1987,     

INFORMATION FOR CONTRIBUTORS

Contributions： The Journal, Acta Mechanica Solida Sinica, is pleased to receive papers from engineers and scientists working in various aspects of solid mechanics. All contributions are subject to critical review prior to acceptance and publication.     

Preface

This special issue of PARTICUOLOGY is devoted to the first UK-China Particle Technology Forum taking place in Leeds, UK, on 1-3 April 2007. The forum was initiated by a number of UK and Chinese leading academics and organised by the University of Leeds in collaboration with Chinese Society of Particuology, Particle Technology Subject Group （PTSG） of the Institution of Chemical Engineers （IChemE）, Particle Characterisation Interest Group （PCIG） of the Royal Society of Chemistry （RSC） and International Fine Particle Research Institute （IFPRI）. The forum was supported financially by the Engineering and Physics Sciences Research Council （EPSRC） of United Kingdom,     

基于鲁棒滤波的捷联导引头视线角速度估计方法

针对捷联导引头无法直接获取视线角速度等信息的问题,研究了鲁棒滤波在大气层外飞行器捷联导引头视线角速度估计中的应用。为了建立非线性滤波估计模型,考虑目标视线角速度的慢变特性,采用一阶马尔科夫模型建立了状态方程;推导了视线角速度的解耦模型,并建立了量测方程;考虑到实际应用中存在系统噪声统计特性失准的问题,基于Huber-Based鲁棒滤波方法,设计了视线角速度滤波器,并完成了基于Huber-Based滤波方法和扩展卡尔曼滤波方法的数学仿真。仿真结果表明Huber-Based滤波方法的视线角、视线角速度及视线角加速度估计精度分别达到0.1140'、0.1423'/s、0.0203'/s2,而扩展卡尔曼滤波方法的视线角、视线角速度及视线角加速度估计精度仅分别为0.6577'、0.6415'/s、0.0979'/s~2。仿真结果证明了该方法可以有效地估计出相对视线角速度等信息,并且在非高斯噪声的条件下,依然可获得较高的估计精度,具有一定的鲁棒性。     

Guide for authors

正Each of the sections below provides essential information for authors.We recommend that you take the time to read them before submitting a contribution to Acta Mechanica Sinica.We hope our guide to authors may help you navigate to the appropriate section.How to prepare a submission This document provides an outline of the editorial process involved in publishing a scientific paper in Acta Mechanica     

Use specification of multiscale materials for life spanned over macro-, micro-, nano-, and pico-scale

Multiscale material intends to enhance the strength and life of mechanical systems by matching the transmitted spatiotemporal energy distribution to the constituents at the different scale, say—macro, micro, nano, and pico,—, depending on the needs. Lower scale entities are, particularly, critical to small size systems. Large structures are less sensitive to microscopic effects. Scale shifting laws will be developed for relating test data from nano-, micro-, and macro-specimens. The benefit of reinforcement at the lower scale constituents needs to be justified at the macroscopic scale. Filling the void and space in regions of high energy density is considered.Material inhomogeneity interacts with specimen size. Their combined effect is non-equilibrium. Energy exchange between the environment and specimen becomes increasingly more significant as the specimen size is reduced. Perturbation of the operational conditions can further aggravate the situation. Scale transitional functions and/or f_j/j+1 are introduced to quantify these characteristics. They are represented, respectively, by , and (f_mi/ma,f_na/mi,f_pi/na). The abbreviations pi, na, mi, and ma refer to pico, nano, micro and macro.Local damage is assumed to initiate at a small scale, grows to a larger scale, and terminate at an even larger scale. The mechanism of energy absorption and dissipation will be introduced to develop a consistent book keeping system. Compaction of mass density for constituents of size 10⁻¹², 10⁻⁹, 10⁻⁶, 10⁻³ m, will be considered. Energy dissipation at all scales must be accounted for. Dissipations at the smaller scale must not only be included but they must abide by the same physical and mathematical interpretation, in order to avoid inconsistencies when making connections with those at the larger scale where dissipations are eminent.Three fundamental Problems I, II, and III are stated. They correspond to the commonly used service conditions. Reference is made to a Representative Tip (RT), the location where energy absorption and dissipation takes place. The RT can be a crack tip or a particle. At the larger size scales, RT can refer to a region. Scale shifting of results from the very small to the very large is needed to identify the benefit of using multiscale materials.