加力燃烧室热声振荡纵向传播特性及控制

建立了管道声传播与不稳定热释放耦合的热声振荡理论模型,并用来对复杂的航空发动机加力燃烧室中的纵向传播的振荡特征频率及稳定性进行分析和预测.利用二维定常计算流体动力学(CFD)模拟结果获得流动平均参数,在此基础上讨论了加力燃烧室内热释放位置、隔热屏穿孔率等结构的变化对热声振荡特性的影响,表明该模型能够方便地应用于对加力燃烧室热声振荡影响因素的研究并揭示某些控制规律.      

分段式固体火箭发动机内部流动不稳定性数值分析

采用大涡模拟技术,针对某分段式固体火箭发动机开展了发动机燃面退移0mm,160mm和280mm三个时刻下发动机燃烧室内部流动不稳定现象的数值分析,获得了三个典型时刻燃烧室内压强可能的振荡特性.计算结果表明,在发动机点火初期燃烧室内流动不稳定性主要由表面涡脱落导致;随着燃面的退移,端面限燃层暴露在燃气中,由于端面包覆结构残余的影响,燃烧室内流动不稳定性主要由障碍涡脱落决定,且与点火初期相比,压强振荡的频率逐步减小.     

航空发动机失稳特征信号甄别

针对航空发动机失稳时的重要表征——喘振信号开展检测、判别和处理方法的研究。通过失稳信号处理器实时获取压气机压力脉动数据,采用时域诊断分析方法完成对失稳信号的在线检测和预警。经压缩部件台架试验验证,失稳信号处理器能成功分离出喘振状态下的失稳信号特征,实现对失稳信号较为准确的捕获,采用的失稳判定方法有效。研究结果表明:失稳特征信号的实时、准确甄别,是发动机失稳主动控制的先决条件,提高失稳特征信号判别的正确率,可有效避免发动机失稳过程中信号的误判、漏判。     

旋转固体火箭发动机飞行器章动不稳定机理述评

针对旋转固体火箭发动机发射小卫星最末级出现的章动现象,分析了其不稳定机理.根据实际观测的飞行数据,分析了飞行器章动不稳定性的特点,给出了几种可能导致飞行器发生侧向角运动的不稳定性机理,并结合实际情况,对各种机理进行了分析.结果显示,飞行器不稳定运动的主要原因是飞行器的质量变化、内部气流的非稳态流动与飞行器姿态运动的相互...     

火星探测器进入阶段稳定性分析

文章针对＂火星探路者＂,对火星探测器在进入火星大气减速过程中的运动稳定性问题进行了研究,分析了质心位置、进入条件、大气参数等因素对火星探测器运动稳定性的影响。分析结果表明,在马赫数大于1.2时,探测器处于一个比较稳定的状态。     

超声速混合层转捩过程实验研究的进展

超声速湍流机理的实验研究是一件十分困难的工作.在2000年以来,本研究小组在低噪声超声速混合层风洞研究、超声速流动精细结构测量技术研究方面取得了重要进展,这给超声速混合层湍流精细结构的研究奠定了基础.为了研究超声速混合层及其气动光学问题,在研制的超声速混合层风洞中,主要以基于纳米技术的平面激光散射技术(Nano-trace Planar Laser Scattering,简称NPLS)为基础,研究了几种对流马赫数的超声速混合层从层流到湍流转捩过程K-H不稳定涡的空间结构,以及K-H不稳定涡的空间结构随着时间的发展过程.实验结果清晰地反映了湍流混合的不稳定性与转捩的精细结构,以及转捩过程的展向精细结构.     

Induction of genomic instability after an acute whole-body exposure of mice to Fe ions

The purpose of this study was to evaluate dose–response relationships for the in vivo induction of micronuclei (MN) as a measure of both initial radiation damage and the induction of genomic instability. These measurements were made in mouse blood erythrocytes as a function of radiation dose, radiation quality, time after irradiation, and the genetic background of exposed individuals. Blood samples were collected from two strains of mouse (CBA/CaJ and C57BL/6J) at different times up to 3 months following a whole-body exposure to various doses of 1 GeV/amu ⁵⁶Fe ions (0, 0.1, 0.5 and 1.0 Gy, at the dose rate of a 1 Gy/min) or ¹³⁷Cs gamma rays (0, 0.5, 1.0 and 3.0 Gy, at the dose rate of 0.72 Gy/min). Blood-smear slides were stained with acridine orange (AO). The frequencies of MN were measured in mature normochromatic-erythrocytes (MN-NCEs) and in immature polychromatic-erythrocytes (MN-PCEs). Effects of both types of radiation on erythropoiesis were also evaluated. As a measure of cell progression delay, a dose-dependent decrease in numbers of PCEs was observed at day 2 post-exposure in both strains, regardless of radiation quality. Subsequently, the levels of PCEs increased in all exposed mice, reaching control levels (or higher) by day 7 post-exposure. Further, at day 2 after the exposure, there was no increase in the frequency of MN-PCEs in CBA/CaJ mice exposed to ⁵⁶Fe ions while the frequency of MN-PCEs elevated as a function of dose in the C57BL/6J mice. At day 4, there was no dose related increase in MN-NCEs in either strain of mouse exposed to ¹³⁷Cs gamma rays. Additionally, at the early sacrifice times (days 2 and 4), ⁵⁶Fe ions were slightly more effective (per unit dose) in inducing MN-NCEs than ¹³⁷Cs gamma rays in CBA/CaJ mice. However, there was no increase in the frequency of MN-NCEs at late times after an acute exposure to either type of radiation. In contrast, both types of radiation induced increased MN-PCEs frequencies in irradiated CBA/CaJ mice, but not C57BL/6J mice, at late times post-exposure. This finding indicates the potential induction of genomic instability in hematopoietic cells of CBA/CaJ mice by both types of radiation. The finding also demonstrates the influence of genetic background on radiation-induced genomic instability in vivo.     

水冲压发动机燃烧稳定性数值研究

建立了水冲压发动机燃烧稳定性计算模型,对一次进水水冲压发动机燃烧室内流场进行数值模拟。研究了燃烧室长度、水燃比、液滴直径等因素对水冲压发动机燃烧稳定性的影响。研究表明,适当增加燃烧室长度、采用多次进水以减小局部水燃比并选取适当的雾化器,有利于水冲压发动机的稳定燃烧。     

Numerical Simulation for the 16 August 1999 EUV Brightenings

The 16 August 1999 EUV brightenings are numerically simulated by a third-order upwind compact scheme, basing on the TRACE observation. The present simulation can give a possible explanation to its formation and evolution. The numerical results show that the initial reconnection jets at around X-point are responsible for the occurrence of EUV brightening. The strong and superposed ejections caused by the first and second coalescence of magnetic islands are possibly related to the lifted material which initially appeared as absorption features and Later EUV-emitting structures respectively. The bi-directional reconnection jets may correspond to the lifted material that either continued to move upward along the apparently open field lines or fell down to the surface.      

引导场对无碰撞电流片低频电磁不稳定性的影响

通过数值求解无碰撞电流片中可压缩磁流体力学模型下得到的一般形式的色散关系,讨论了无碰撞电流片中引导场对低频电磁波不稳定性的影响.结果表明,平衡态磁场中的引导场,对于三维扰动传播的波不稳定性有很强的影响.(1)在电流片中间平面上(z=0),无引导场时,没有不稳定性发生,但若存在引导场,不稳定性便发生,并随着引导场的增强,不稳定性明显增强,不稳定的波模可能是低混杂模.(2)在中间平面附近(z=0.2),电流片是不稳定的.随着引导场的增强,不稳定性增长率明显地增强,不稳定的波模从平行和反平行两个方向传播变为反平行方向一个方向传播,并且是斜传播的,具有低频哨声模或低混杂模的特征.(3)在电流片边缘附近(z=0.8),引导场对不稳定的波模和增长率没有明显影响,不稳定的波模都是准平行的哨声波.