航天器推进系统管路充填过程动态特性(Ⅱ)实验模拟与结果评估

针对某一具有工程背景的卫星推进系统,建立了一个包括抽真空设备的实验模拟系统,以水为介质进行真空充填过程实验研究,结果表明充填过程中存在较强水击;利用数学模型对实验室系统充填过程进行仿真,计算结果与实验测量值吻合,表明模型仿真是可靠的。     

内螺旋花键冷挤压成形工艺

介绍了某产品齿轮挡块 45°内螺旋花键的冷挤压成形工艺，包括模具设计及试验过程。     

等温锻造Ti—47Al—2Cr—1Nb合金显微组织细化机理

Ti 4 7Al 2Cr 1Nb(at % )合金经等温锻造形变热处理后 ,显微组织得到显著细化 ;TEM分析表明 ,TiAl合金在等温变形时 ,形变主要以γ相板条内产生变形孪晶的方式进行 ;大部分变形孪晶垂直于α2 /γ界面 ,热处理时易形成再结晶核心 ,形成等轴γ晶粒     

3D-C/SiC复合材料拉-拉疲劳模量和电阻的变化

在室温最大应力为250MPa，应力比R＝0．1和频率为60Hz条件下，对3D－C／SiC复合材料进行了拉－拉疲劳试验。用共振法和电阻增量仪分别测试了杨氏模量及电阻的变化。结果表明：随循环次数增加，杨氏模量呈显著下降，缓慢下降和突然下降的变化规律。杨氏模量的下降大部分发生在疲劳循环的前600次。缓慢降低阶段约占疲劳寿命的94％以上，此阶段杨氏模量变化率与循环次数的对数近似呈线性关系，电阻变化率除首次循环降低外，随着循环次数增加一直在增加。增加规律大致可分为缓慢增加，台阶式增加和急剧增加三个阶段。材料的电阻变化率基本反映了纤维的损伤程度和破坏形式，可作为表征复合材料纤维损伤的有效参量。     

利用多普勒原理测量微机电系统中微结构的动态特性

介绍了将显微扫描激光多普勒测振仪与基础激振法相结合的微结构动态特性的非接触无损测量方法、扫描激光多普勒测振仪的工作原理、设计的基础激振器及其驱动信号.并给出典型微结构--微悬臂梁的测量结果.测量结果与理论计算及有限元仿真结果相符,验证了该方法的有效性.     

基于动力学仿真技术的TC4整体叶轮铣削参数优化

针对某航空发动机TC4整体叶轮在数控加工过程中存在颤振、加工效率低及因加工变形而导致局部超差等问题,提出了相应的铣削参数优化解决方案。在进行切削力系数辨识试验获取TC4材料的切削力系数及锤击试验获取加工系统动力学特性参数的基础上,通过综合使用自行开发的铣削加工动力学仿真软件SimuCut和国外的CutPro软件进行动力学仿真与优化,获得了优化的切削参数。使用优化的切削参数进行加工,有效地消除了颤振和因加工变形引起的局部超差,提高了加工效率。     

Practical compensation for nonlinear dynamic thrust measurement system

The real dynamic thrust measurement system usually tends to be nonlinear due to the complex characteristics of the rig, pipes connection, etc. For a real dynamic measuring system,the nonlinearity must be eliminated by some adequate methods. In this paper, a nonlinear model of dynamic thrust measurement system is established by using radial basis function neural network(RBF-NN), where a novel multi-step force generator is designed to stimulate the nonlinearity of the system, and a practical compensation method for the measurement system using left inverse model is proposed. Left inverse model can be considered as a perfect dynamic compensation of the dynamic thrust measurement system, and in practice, it can be approximated by RBF-NN based on least mean square(LMS) algorithms. Different weights are set for producing the multi-step force, which is the ideal input signal of the nonlinear dynamic thrust measurement system. The validity of the compensation method depends on the engine’s performance and the tolerance error0.5%, which is commonly demanded in engineering. Results from simulations and experiments show that the practical compensation using left inverse model based on RBF-NN in dynamic thrust measuring system can yield high tracking accuracy than the conventional methods.     

基于检测结果的涡轮叶片精铸型腔反变形优化设计

针对空心涡轮叶片精铸过程中的试错法和数值仿真法难以敏捷反应铸件的真实变形情况,提出一种基于检测结果的精铸零件反变形综合补偿方法.通过对精铸叶片试模样件进行三坐标检测及统计分析,得到叶身截面收缩、扭转和弯曲变形情况,并建立其综合补偿反变形模具型腔优化算法,实现精铸型腔的反变形优化设计.以精铸叶片试模样件叶尖处截面为例,其叶身段型面误差、前缘最大误差、后缘最大误差相对于未补偿前分别减少了50%,68%和31%.实例验证表明:其研究成果能有效提高空心涡轮叶片的精铸成型精度,达到精确控形的目的.      

基于EFFD方法的自然层流短舱优化设计

采用extended free-form deformation(EFFD)方法研究了自然层流(natural laminar flow,NLF)短舱的气动外形优化设计方法.使用基于Bernstein基函数的EFFD方法完成了NLF短舱剖面的参数化,利用基于k-εSST(shear stress transport)两方程湍流模型的γ-θ转捩模型进行自然转捩预测,结合EFFD、一种混合动网格方法、Kriging代理模型和改进的粒子群算法(particle swarm optimization,PSO)建立了针对NLF短舱气动外形的优化设计框架.采用该框架分别对通气NLF短舱和带动力NLF短舱进行优化设计.单独通气NLF短舱优化结果的外表面实现48%的层流,阻力系数比初始通气NLF短舱减小了0.0003.带动力NLF短舱的优化结果外表面保持了41%的层流.这些结果表明采用相关技术建立的优化设计框架在NLF短舱设计中具有一定应用价值.     

Friction moment analysis of space gyroscope bearing with ribbon cage under ultra-low oscillatory motion

This paper presents the model of calculating the total friction moment of space gyroscope ball bearings which usually work under ultra-low oscillatory motion and are very sensitive to the friction moment. The aim is to know the proportion of the friction moment caused by each frictional source in the bearing＇s total friction moment, which is helpful to optimize the bearing design to deduce the friction moment. In the model, the cage dynamic equations considering six degree-of-freedom and the balls dynamic equations considering two degree-of-freedom were solved.The good trends with different loads between the measured friction moments and computational results prove that the model under constant rate was validated. The computational results show that when the speed was set at 5 r/min, the bearing＇s maximum total friction moment when oscillation occurred was obviously larger than that occurred at a constant rate. At the onset of each oscillatory motion, the proportion of the friction moment caused by cage in the bearing＇s total friction moment was very high, and it increased with the increasing speed. The analyses of different cage thicknesses and different clearances between cage pocket and ball show that smaller thickness and clearance were preferred.