静电陀螺转子径向偏心干扰力矩分析

推导了静电陀螺仪转子径向偏心产生的静电场干扰力矩计算公式，计算分析了该干扰力矩产生的陀螺漂移，其结果对静电陀螺仪的设计与研制具有参考价值。     

壳体旋转对由恒速磁场引起的漂移误差的调制作用

陀螺仪通过外加旋转磁场恒速时,如果磁场旋转轴与转子动量矩轴不重合,将产生干扰力矩引起自由转子陀螺仪的漂移误差。文中建立了壳体翻滚的运动坐标系,分析了静止坐标系、平台坐标系、壳体坐标系、光电传感器坐标系之间的运动关系;最后从理论上证明了壳体旋转对该项漂移误差的调制作用。分析结果对于研制静电陀螺仪壳体旋转系统具有一定的参考价值。     

差动式电感传感器最小电磁吸力矩的优化设计

本文采用复形法对某型船用挠性陀螺仪的差动式电感传感器进行了最小电磁吸力矩的优化设计，找出线圈匝数和激磁电压的最优值。研究表明，采用合适的线圈匝数和激磁电压，可使电磁吸力矩减小一个数量级以上，从而大大减小挠性陀螺仪的漂移。     

改进小波阈值法在MEMS陀螺信号去噪中的应用

陀螺随机漂移是影响MEMS陀螺仪精度的重要指标,有效减小MEMS陀螺仪的随机漂移误差是提高MEMS陀螺仪使用精度的关键技术之一.文中在分析了小波阈值法的去噪原理和存在的缺陷的基础上,构造了一种新的阈值函数,并利用3σ准则提取阈值,提出了一种改进的,小波阈值去噪法,并将其应用于MEMS陀螺仪输出信号的滤波处理中,取得了良好的去噪效果.实验结果表明,文中提出的方法可以有效减少信号中的高频噪声,很好地抑制MEMS陀螺仪的随机漂移,去噪效果明显优于传统的,小波阈值法.     

短路匝式角度传感器不同极数下输出特性对比分析

针对短路匝式角度传感器多极结构与其输出特性之间关系的问题,对比分析了四极、八极、十二极和十六极短路匝式角度传感器的输出特性参数。首先,通过对短路匝式角度传感器多极结构和工作原理的分析,建立了其输出特性与极数之间的方程式。其次,利用ANSYS Maxwell-3D软件对四极、八极、十二极和十六极短路匝式角度传感器的输出特性进行了仿真分析,得到了不同极数下传感器输出极内磁通量和输出电压的对比曲线。最后,通过搭建短路匝式角度传感器输出特性的实验测试平台,得到了其输出电压的实测结果,与仿真分析结果进行了对比。结果表明,极数大于八极的短路匝式角度传感器的制造和应用是没有实际意义的,且八极传感器工作在±4°内具有高的线性度和对称度。     

基于小波分析与LSSVM的陀螺仪随机漂移建模

为了提高陀螺仪的使用精度,以陀螺仪随机漂移时间序列为研究对象,建立了基于小波分析和最小二乘支持向量机（LSSVM）的陀螺仪随机漂移模型。陀螺仪作为高精度敏感器件,其随机漂移信号具有非线性、弱平稳性等特点,难以补偿。为了提高补偿精度,这里采用小波分析对陀螺仪随机漂移信号进行多尺度分解,利用最小二乘支持向量机方法对重构后的近似序列和细节序列建立非线性子模型,最后将各子模型输出融合作为组合模型输出。最后将该算法用于动调陀螺仪的随机漂移建模,实验结果表明基于该组合算法的非线性模型能够有效地反映陀螺仪的随机漂移特性,建模效果明显优于直接采用LSSVM和ANN建立的模型。     

静电陀螺监测器中静电陀螺仪的漂移误差模型

本推导了静电陀螺仪转子动量矩的运动方程,根据此方程并应用向量场理论,将造成静电陀螺漂移的外部干扰力矩划分为守恒力矩和非守恒力矩两部分。按照进动规律,最终得到静电陀螺监控器中陀螺仪漂移误差模型的全量形式。     

控制陀螺仪与g 2 / 有关干扰力矩的主要技术途径

一高精度液浮陀螺仪中一般都使用动压气体轴承，动压气体轴承的不等刚度及转子姿态角是陀螺仪ｇ２有关干扰力矩的主要来源，加之由于径向轴承的位移和转子姿态角的出现使问题更加复杂。本文假定框架等刚性的前提下，着重讨论动压气体轴承的某些参数对单自由度液浮陀螺仪与ｇ２有关干扰力矩的影响及其控制此项干扰力矩的技术途径。     

小型静电陀螺仪转子变形及干扰力矩分析

推导了小型静电陀螺仪转子非球形干扰力矩公式，仿真分析了两种不同结构的实心转子的温度变形、离心变形、压力变形及综合变形，计算了其变形产生的干扰力矩及漂移。     

基于位置信号的三浮陀螺仪有源磁悬浮干扰力矩补偿方法

针对高精度三浮陀螺采用有源磁悬浮之后带来新的干扰力矩问题,提出了基于位置信号的干扰力矩补偿法。对有源模式下径向元件电磁模型进行了分析,得出磁悬浮干扰的直接原因为同一坐标方向的两个极下磁场不对称,定、转子几何中心偏移越大这种不对称性也越大。建立了磁悬浮干扰力矩常值部分和随机部分与定中位置、定中精度的关系数学模型,在陀螺测试输出中对其进行补偿。多次实验表明,引入该补偿算法后陀螺固定位置随机漂移精度平均提高了33%~42%,同时也提高了磁悬浮的定中精度,证明此方法有效。     

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.