环形激光陀螺随机误差测试中的计数误差

详细讨论了环形激光陀螺（RLG）误差测试中的计数误差。首先提出了在角度随机游走为主要误差源的情况下，RLG的离散输出模型。在假设累积角度量化误差为白噪声的前提下推导了方差（或AIlan方差）分析中的量化误差模型。接着指出白噪声假设并不总能成立，特别是对于由计数器只能计整数引致的量化误差（特称为“计数误差”），由于量化间隔很大，这一假设通常不能成立。最后，给出了一种白噪声假设不能成立时的处理方法及仿真数据分析结果。     

感应同步器鉴幅测角系统静态误差分析及关键电路设计

本文系统论述了采用感应同步器进行角位置测量的连续绕组激磁，分段绕组输出的鉴幅方案，对这个方案的工作原理进行介绍，并对此方案产生的静态误差进行分析，给出减小误差的方法，最后得出相关结论。     

结构误差造成的半球谐振陀螺闭环检测误差分析

半球谐振陀螺是一种具有广阔应用前景的高精度陀螺。由于制造工艺和装配过程中的因素，其结构难免会出现误差。根据闭环检测机理，推导出结构误差的数学表达式，分析了它对测量结果的影响，这对于编制软件算法以补偿结构误差具有一定的指导意义。     

船用惯性导航系统姿态测量误差辨识及其补偿方法研究

本文分析了某型号船用惯性导航系统（ＳＩＮＳ）的试验数据，结果表明，ＳＩＮＳ的姿态误差主要来源于水平测姿传感器。据此，本文对该ＳＩＮＳ水平姿态测量误差的辨识及其补偿方法进行了研究，并建立了水平测姿误差的回归数学模型，以提高ＳＩＮＳ姿态精度     

考虑信号处理特性的划摇算法优化

捷联惯导系统一般用划摇算法来补偿其速度漂移,标准的划摇算法是以理想的陀螺和加表信号为输入设计的,而实际中常用数字滤波器处理激光陀螺和加表信号,由于滤波器的非理想性,滤波后信号的幅频特性发生畸变,引入了较大的划摇算法误差。参考标准划摇算法误差公式,用相对划摇误差分析方法比较研究了算法的误差变化特性,证明误差大小与滤波器通带特性有关。基于经典划摇运动,推导了数据滤波后优化的划摇算法公式。修正算法考虑了滤波器幅频特性的影响,补偿了滤波器引入的划摇算法误差。仿真表明:优化算法在保证滤波器较小延时的同时,能明显减小算法精度损失,提高导航算法整体精度水平。     

小型静电陀螺仪电极面积及电极装配误差研究

介绍了小型静电陀螺仪的电极支承结构和电极面积误差引起的干扰力矩的计算公式,并根据影响电极面积的各种因素推导出了电极面积的误差范围。根据装配误差产生干扰力矩的情况确定了最终的装配精度,为电极的设计提供了重要的参考依据。     

水下爆炸压力测量中的若干问题

本文简要叙述了水下爆炸时的物理现象及爆炸产生的冲击波测量方法,详细分析了测试系统中各种因素对测量的影响及实测时避免的方法。     

ADAPTIVE MESHLESS METHOD BASED ON LOCAL FIT TECHNOLOGY

An h-adaptive meshless method is proposed in this paper. The error estimation is based on local fit technology, usually confined to Voronoi Cells. The error is achieved by comparison of the computational results with smoothed ones, which are projected with Taylor series. Voronoi Cells are introduced not only for integration of potential energy but also for guidance of refinement.New nodes are placed within those cells with high estimated error. At the end of the paper, two numerical examples with severe stress gradient are analyzed. Through adaptive analysis accurate results are obtained at critical subdomains, which validates the efficiency of the method.     

Molecular-dynamics of a 2D Model of the Shape Memory Effect

This work investigates the thermodynamic properties of a qualitative atomistic model for austenite–martensite transitions. The model, still in 2D, employs Lennard-Jones potentials for the determination of the atomic interactions. By use of two atom species it is possible to identify three stable lattice structures in 2D, interpreted as austenite and two variants of martensite. The model is described in the first part of the work [6] in detail. The present work studies the thermodynamic properties of the model concerning a small, 2-dimensional test assembly consisting of 41 atoms. The phase stability is investigated by exploitation of the condition of minimal free energy. The free energy is calculated from the thermal equation of state, which is measured in numerical tensile tests. In the second part of this work a chain of eleven 41-atom assemblies is investigated. The chain is interpreted as an idealized larger body, where the individual crystallites represent crystallographic layers allowing for the creation of micro structure. By use of tensile tests at various temperature conditions we sketch how such chain may exhibit quasi-plasticity, pseudo-elasticity and the shape memory effect.     

Kinetics of phase transformations in the peridynamic formulation of continuum mechanics

We study the kinetics of phase transformations in solids using the peridynamic formulation of continuum mechanics. The peridynamic theory is a nonlocal formulation that does not involve spatial derivatives, and is a powerful tool to study defects such as cracks and interfaces.We apply the peridynamic formulation to the motion of phase boundaries in one dimension. We show that unlike the classical continuum theory, the peridynamic formulation does not require any extraneous constitutive laws such as the kinetic relation (the relation between the velocity of the interface and the thermodynamic driving force acting across it) or the nucleation criterion (the criterion that determines whether a new phase arises from a single phase). Instead this information is obtained from inside the theory simply by specifying the inter-particle interaction. We derive a nucleation criterion by examining nucleation as a dynamic instability. We find the induced kinetic relation by analyzing the solutions of impact and release problems, and also directly by viewing phase boundaries as traveling waves.We also study the interaction of a phase boundary with an elastic non-transforming inclusion in two dimensions. We find that phase boundaries remain essentially planar with little bowing. Further, we find a new mechanism whereby acoustic waves ahead of the phase boundary nucleate new phase boundaries at the edges of the inclusion while the original phase boundary slows down or stops. Transformation proceeds as the freshly nucleated phase boundaries propagate leaving behind some untransformed martensite around the inclusion.