气动参数对后台阶三维缝隙换热影响的研究

针对涡轮叶片尾缘冷却结构特点,建立了后台阶三维缝隙结构气膜冷却特性试验台,测量了缝隙中心和肋中心下游换热系数的局部分布,研究了不同雷诺数Re(5000~15000)与吹风比Br(0.5~2.0)对换热系数的影响规律,试验结果表明:(1)出口的换热系数总体呈下降趋势,但在肋后中心线略有起伏;(2)随着Re的增大,换热系数增大,随着Br的增大,换热系数减小;(3)在靠近出口位置,由于热边界层与三维掺混特性流场的影响,使得换热变得复杂。     

Microstructure and Optical Characterization of Magnetron Sputtered NbN Thin Films

Some fundamental studies on the preparation, structure and optical properties of NbN films were carried out. NbN thin films were deposited by DC reactive magnetron sputtering at different N2 partial pressures and different substrate temperatures ranging from –50 ℃ to 600 ℃. X-ray diffraction analysis (XRD) and scanning electron microscopy (SEM) were employed to characterize their phase com- ponents, microstructures, grain sizes and surface morphology. Optical properties inclusive of refractive indexes, extinction coefficients and transmittance of the NbN films under different sputtering conditions were measured. With the increase in the N2 partial pressure, δ-NbN phase structure gets forming and the grain size and lattice constant of the cubic NbN increasing. The deposited NbN film has relatively high values of refractive index and extinction coefficient in the wavelength ranging from 240 nm to 830 nm. Substrate tem- perature exerts notable influences on the microstructure and optical transmittance of the NbN films. The grain sizes of the δ-NbN film remarkably increase with the rise of the substrate temperature, while the transmittance of the films with the same thickness decreases. Ultra-fine granular film with particle size of several nanometers forms when the substrate is cooled to –50 ℃, and a remarkable aug- mentation of transmittance could be noticed under so low a temperature.     

基于CCD的底片判读仪透射屏厚度精确测量

提出了一种利用线阵CCD传感器作为接收装置，以8253编程芯片实现自动测量并实时显示测量结果的底片判读仪透射屏厚度测量系统。文中主要论述了该系统的工作原理和软硬件的实现途径，并分析了系统的测量误差；文章最后列出了实测数据，证明了系统的可行性和先进性。     

Kevlar/Nomex蜂窝夹层结构表面粘贴镀铜箔聚酰亚胺薄膜的工艺研究

文章对Kevlar面板Nomex蜂窝夹层结构表面粘贴镀铜箔聚酰亚胺薄膜的工艺进行了研究,分析了工艺特点、工艺流程、工艺难点,以及针对工艺难点所采取的工艺措施,最后根据产品的研制情况给出结论。     

飞机用固体膜润滑剂

针对新机种对固体膜润滑剂的需求,研制了两种固体膜润滑剂-HR-7201和HR-7101.润滑剂采用国产原材料,具有摩擦系数低,耐高低温及耐介质等优良性能,使用温度HR-7201为-60～300℃,HR-7101为-60～200℃,短期可到250℃.已通过飞机典型零部件试验及长期试车考核,并在飞机上应用.     

薄膜材料和纤维材料的热扩散率测量

介绍了激光热波技术用于测量薄膜材料和纤维材料热扩散率的测试系统，测试温度范围为２０－５００℃。讨论了测量中的各种试验条件、基本公式和误差分析。在理论上此系统可以应用于任何厚度样品面向热扩散率的测量。     

冷轧机补偿原理及其控制算法

液压压下控制系统是冷连轧机控制系统中十分重要的组成部分,它主要实现机架辊缝大小的控制,对于轧制板材的板形有着直接的影响.在轧制过程中,由于轧辊偏心(包括工作辊和支撑辊)、油膜厚度的波动、轧机的弹跳等因素.为了解决这些问题,对于液压压下控制系统中存在的偏心补偿、油膜补偿和弹跳补偿进行了深入的理论分析,研究了冷连轧机液压压下控制系统中偏心补偿、油膜补偿、弹跳补偿的数学模型、实现过程,并与国内外相关理论进行了对比,阐述了各自的优缺点.     

带密布气膜冷却孔的涡轮叶片等效应力分析方法研究

以带气膜冷却孔的航空燃气涡轮发动机涡轮叶片为研究背景,引入了等效概念对密布小孔结构进行了详细的应力-应变分析。这种等效分析方法是把多孔材料转化为具有等效材料常数的等效实体材料。根据MARC大型通用软件的线弹性及弹-塑性有限元应力分析结果,将小孔效应转化为等效弹性常数及等效应力-应变曲线。最后以某发动机高压涡轮工作叶片为例,将得到的等效材料参数引入到叶片的有限元强度计算中,从而得到考虑密布孔影响的涡轮叶片应力应变场,并通过子模型计算得到更为准确的孔边最大应力。     

数据格式转换技术在精密测量中的应用

叙述了为提高数据传输可靠性,在接收精密仪器所采集的数据过程中考虑将原有RS232串口通信,改进为USB接口通讯。但是接收到的信号出现了不明原因的周期性强干扰。为此,通过分析USB/RS232转换原理及A/D采集输出数据特点,对原软件的数据采集部分增补了具有特殊功能的子程序,使得应用程序可以自行恢复数据的完整性。此方法具有通用性,可在不同软件编辑环境中实现,且不影响硬件组成。文中又详细介绍了在薄膜厚度在线测量中应用上述USB接口通信的情况,实测结果表明试验取得了预想的效果。改进后的电容测量系统具有更为广泛的应用前景。     

Kinetic Monte Carlo Simulation of EB-PVD Film:Effects of Substrate Temperature

The 2D kinetic Monte Carlo (KMC) simulation was used to study the effects of different substrate temperatures on the microstruc-ture of Ni-Cr films in the process of deposition by the electron beam physical vapor deposition (EB-PVD). In the KMC model, substrate was assumed to be a “surface” of tight-packed rows, and the simulation includes two phenomena: adatom-surface collision and adatom diffusion. While the interaction between atoms was described by the embedded atom method, the jumping energy was calculated by the molecular static (MS) calculation. The initial location of the adatom was defined by the Momentum Scheme. The results reveal that there exists a critical substrate temperature which means that the lowest packing density and the highest surface roughness structure will be achieved when the temperature is lower than the smaller critical value, while the roughness of both surfaces and the void contents keep decreasing with the substrate temperature increasing until it reaches the higher critical value. The results also indicate that the critical substrate temperature rises as the deposition rate increases.