阻拦系统动力学建模与仿真

 以Mark 7 Mod 1型阻拦系统为基础,借助其中的油液流量系数的经验公式,将其扩展到Mark 7 Mod 3型阻拦系统。首先,将K-5型凸轮曲线进行扩展,重新设计凸轮曲线,使主液压缸的行程增加到4.65 m,进而增加了阻拦系统的容量,实现阻拦系统的优化。其次,考虑到主液压缸的质量不能被忽略,通过引入绳索的弹性形变,实现了阻拦过程主液压缸惯性、滑轮缓冲装置的惯性和飞机惯性的综合动力学仿真。再次,增加了滑轮缓冲系统,使阻拦系统的液压模型更为准确、完整。最后,在考虑了凸轮阀控制曲线以及锥形阀流量系数等各项参数变化的情况下,研究飞机各状态与阻拦系统中各参数的相互影响情况。     

Numerical investigation of the nonreacting and reacting flow fields in a transverse gaseous injection channel with different species

The mixing and combustion process has an important impact on the engineering realization of the scramjet engine. The nonreacting and reacting flow fields in a transverse injection channel have been investigated numerically, and the predicted results have been compared with the available experimental data in the open literature, the wall pressure distributions, the separation length, as well as the penetration height. Further, the influences of the molecular weight of the fuel and the jet-to-crossflow pressure ratio on the wall pressure distribution have been studied. The obtained results show that the predicted results show reasonable agreement with the experimental data, and the variable trends of the penetration height and the separation distance are almost the same as those obtained in the experiment. The vapor pressure model is suitable to fit the relationship between the penetration height, the separation distance and the jet-to-crossflow pressure ratio. The combustion process mainly occurs upstream of the injection port, and it makes a great difference to the wall pressure distribution upstream of the injection port, especially when the jet-to-crossflow pressure ratio is large enough, namely 17.72 and 25.15 in the range considered in the current study. For hydrogen, the combustion downstream of the injection port occurs more intensively, and this may be induced by its smaller molecular weight.     

固体火箭发动机磁悬浮试验架系统动态性能分析

在磁悬浮系统数学模型的基础上,将磁悬浮试验架对发动机的悬浮支承等效为质量一弹簧．阻尼系统。计算了磁悬浮试验架的刚度、阻尼及固有频率,计算结果得到了试验的验证。表明除系统机械设计参数外,控制方式及控制器参数是影响系统动态特性的关键因素,并通过仿真说明了控制器参数对系统动态性能的影响。为设计适合发动机试验的磁悬浮系统提供参考。     

复杂载荷下偏心穿透裂纹应力强度因子的计算方法

提出了三维矩形平板内偏心穿透裂纹承受复杂非线性载荷下,仅含有3个系数的通用权函数。采用有限元法获得了三维矩形平板裂纹体模型下的3组参考应力强度因子,结合二元拉格朗日插值法获得了通用权函数系数。进行了自洽性验证以及裂纹面上承受简单3次、5次、7次、复杂幂函数应力分布和残余应力分布下通用权函数的验证。结果表明,通用权函数的自洽性误差在0.9%以内;裂纹面上承受复杂幂函数应力分布时,通用权函数法的误差在4.5%以内;裂纹面承受残余应力分布载荷时,通用权函数法的误差在8.5%以内。说明所提出的通用权函数具有较高的计算精度,可以满足工程中高效、准确地计算偏心穿透裂纹承受任意复杂非线性载荷下的应力强度因子需求。      

Libration and end body swing stabilization of a parallel partial space elevator system

This paper studies the libration and stabilization of a parallel partial space elevator system in circular orbits. The system is made up of two paralleled partial space elevators, each of which consists of one main satellite, one end body and a climber moving along the tether between them. The libration characteristics of the elevator are studied through numerical analysis by a new dynamic model, and a novel control strategy is proposed to stabilize the swing of the end body by projecting the climber speeds only. Optimal control method is used to implement the new control strategy in the case where the climbers move in opposite direction. The simulation results validate the effectiveness of the proposed control strategy whose application will neither sacrifice the transport efficiency nor exacerbate libration significantly.     

供氧模式对载人航天器气压控制的影响分析

载人航天器气压控制系统主要负责控制密封舱内氧分压和总压满足指标要求,承担长期载人任务的载人航天器通常配备电解制氧系统用于维持密封舱内氧分压水平。文章建立了一种载人航天器密封舱气压控制系统仿真分析模型,利用该模型分析对比了氧气瓶供氧和电解制氧供氧2种模式对应的密封舱氧分压和总压变化规律。结果表明,驻留24 h内,氧气瓶供氧模式对应的氧分压单调下降;电解制氧供氧模式对应的氧分压并非单调下降,而是取决于供氧速率与乘员代谢耗氧间的关系,且氧分压变化范围要远小于氧气瓶供氧模式。驻留60 d内,电解制氧供氧模式对应的氧分压在上下限间的变化周期以及总压的变化周期要明显长于氧气瓶供氧模式。为避免空气温度的影响,氧分压和总压的控制范围应比允许范围窄。     

磁悬浮飞轮位移传感器谐波扰动的主动抑制

针对磁悬浮飞轮转子位移传感器谐波噪声引起的多频扰动问题,提出了一种基于级联相移陷波器的全转速自适应控制方法。首先根据多频扰动特性,构造分级的自适应相移陷波器,每级陷波器对应一个陷波频率;然后,将陷波器级联,分别设置相角补偿矩阵解决闭环控制回路在全转速范围内的稳定性问题。最后,以五自由度磁悬浮飞轮为实验对象进行实验验证,实验结果表明,所提出算法能够在全转速范围内有效地抑制谐波扰动。     

汽车主动悬架的仿真研究

通过车辆主动悬架模型的建立,采用状态反馈配置极点方法确定主动悬架的控制方法,并在MAT-LAB/S imu link环境中对其进行仿真,仿真结果表明该方法具有很好的效果。     

偏微分方程组的一种化简方法

以李群为工具,给出了一种化简两个自变量,两个未知函数的一阶偏微分方程组的方法,在一定条件下,可将偏微分方程组化简为一个阶偏微分方程,若能求出此一阶偏微分方程的解,则只需再解一个一阶常微分方程,即可得出原偏微分方程线的解,该方法可用于某些一阶偏微分方程组的求解,其中包括非定常完全气体一维均熵方程和波动方程。