燃烧室内不良流线体挂火问题的分析

本文介绍了在冲压发动机燃烧室试验中出现的喷嘴环挂火现象,指出了挂火的特点;分析了火对临界推力的影响;对产生挂火的主要原因进行了剖析,提出了尾迹分离流是造成火焰前传的原因;最后列举了解决挂火问题的方法.     

弹性支撑条件下齿轮体的动力特性与啮合齿的动力响应

 结合齿轮的实际工作状况，建立了齿轮结构的弹性体动力学模型，进行了弹性动力学分析,得出了齿轮的弹性固有特性; 考虑了弹性支撑轴对齿轮体振动的影响，将其处理为弹性支撑，推导了弹性支撑弹簧刚度的表达式,并在弹性边界条件下，考虑了弹性圆盘对啮合齿响应的影响，建立了齿轮支撑系统的动力模型和轮齿响应计算模型，研究了齿轮支撑系统的固有特性,并与实验结果进行了对比验证; 求解了啮合齿的动力学响应，并进行了模拟仿真。研究表明采用弹性支撑条件进行齿轮支撑系统分析是真实、精确的，为齿轮弹性体的动载荷计算、动态设计和齿轮传动系统的精确动力学研究提供了一种分析方法。     

扰流板式畸变模拟装置的数值计算及人工神经网络建模

数值计算了用于某型空中试车台吊舱的扰流板式畸变模拟装置,应用总压恢复系数、周向畸变指数评价了该装置的畸变效果并与试验数据进行了对比分析,为后续发动机在空台上确定临界畸变指数及敏感系数提供了可用量值的参考.根据部分计算数据,建立了该扰流板式畸变模拟装置的人工神经网络模型,并预估了12个状态的畸变模拟效果,验证了该人工神经网络模型的有效性,为减少试验点数节省试验经费提供了有效的途径.     

基于FPGA和DSP的光电吊舱控制系统设计与实现

本文介绍了机载两框架两轴光电吊舱的工作原理,并设计了一种基于FPGA和DSP的光电吊舱控制系统,充分利用了FPGA和DSP的各自优势,提高了系统的响应速度。详细描述了控制系统硬件电路的功能划分和实现过程。提出了控制回路设计方案,并通过实验验证了控制系统的性能,在两框架两轴光电吊舱上实现了较高的光轴稳定精度     

航天器电缆网快速协同设计方法及关键技术

以航天器电缆网传统研制模式的局限性为出发点,提出了电缆网全息模型的概念及其通用模型体系,实现了包含全要素设计信息的完整产品数字化定义;基于先"修路"后布线的设计理念,系统地提出了导航式电缆网快速协同设计方法及其相关算法,建立了航天器整器级统一的电缆网络通道"地图",有效增强了电缆网的顶层设计,减少了每束电缆并行设计时路径统筹规划不够和走向不优化的问题;构建了电缆网机电一体化协同模式和面向研制全周期的一体化业务流程,建立了跨型号跨专业的通用模型库、参数库、算法与规则库,完善了电缆网系统级设计和底层数据模型,实现了不同专业间的并行协同;开发了导航式电缆网快速协同设计系统,实现了基于参数驱动的复杂电缆网快速三维布线,提升了设计效率效益,并在以空间站为代表的载人航天型号中开展了应用,为复杂电缆网的研制提供了一种有效方法和手段。     

机械设计基础课虚拟实验的设计与开发

阐述了机械设计基础课程虚拟实验的主要功能和特点.提出了建立基于网络的虚拟实验体系内容.采用Solidworks、3Dmax、Flash开发的机构运动简图演示、机构运动测绘和减速器拆装等虚拟实验,大大提高了实验效率,解决了设备、教具不足的矛盾.打破了教师传统的示范演示,实现了教生互动,激发了学生学习的主动性,促进了教学效率和质量的提高.     

某小型涡轮喷气发动机改进设计

某型中程、中高空无人飞行器研制对动力装置提出了更高的性能要求.对某型涡轮喷气发动机进行了改进、改型设计.在结构和性能等方面采用了多项技术改进措施,提高了发动机的1次连续运行时间,延长了累计使用寿命,并使发动机的增压比、绝热效率和空气流量都得到了不同程度的提高;对第1级压气机转子重新进行了全三维气动设计,改善了压气机部件性能,增大了发动机在最大转速下的推力,降低了发动机的单位耗油率.     

气体挤压膜悬浮平台的研究方法

利用流体动力润滑理论阐述了挤压膜悬浮平台的可能性,在润滑工况假设方面提出了周期化的思想,在解决非定常雷诺方程时利用了周期化的初始条件,大大减少了非定常雷诺方程的运算量,并提高了收敛速度。最后给出了利用简单的实验装置给予挤压膜悬浮初步验证的方法。     

PHM技术在机载机电执行部件中的应用研究

介绍了 PHM 技术的概念和功能。研究了对 PHM 技术在机载机电执行部件中的应用。设计了 PHM 系统的功能框图,探索了如何实现对 PHM 系统预测推理方法。表明了 PHM 技术在机载机电执行部件中有着广阔的应用前景。     

直升机机身外形对气动特性的影响

基于FLUENT流体力学软件,进行了直升机机身流场的数值模拟和分析。描述了网格生成方法,给出了计算迭代步骤和流程图。针对ROBIN机身绕流场进行了计算,并与可得到的实验结果进行了对比,验证了计算结果的可靠性。在此基础上,以NUAA模型机身为算例,改变机身尾部、截面和头部形状对其流场进行了对比计算,给出了表面压强系数分布、机身阻力等计算结果,讨论了直升机机身外形参数对气动特性的影响,得出了一些有意义的结论。     

高强高韧Al-Cu-Li-Mg-Zr-Zn-Mn合金热变形行为

在Gleeble～1500热模拟实验机上，采用高温等温压缩，应变速率为0．001～10／s，变形温度为360～520％，对通用型铝锂合金在高温压缩变形中的流变应力行为进行了研究，分析了其高温变形的物理本质。结果表明：在等应变速率下，真应力随温度的升高而降低；在相同的变形温度下，随应变速率的增加，流变应力水平升高。在较低的变形速率及较高的变形温度条件下热变形时，通用型铝锂合金容易发生动态再结晶。而变形速率较高，变形温度较低时，通用型铝锂合金可能发生剪切变形，热变形过程中则主要发生动态回复。     

P2P模式的系统结构研究

本文首先介绍了什么是P2P和它的基本运作模式。详细阐述P2P模式的主要形式及其相应的系统结构。     

通用型大气数据计算机自动测试系统的研制

针对我军用飞机大气数据计算机的测试问题,在全面分析了国产及俄制大气数据计算机测试需求的基础上,采用PCI总线技术,提出了一种满足系统测试需求的通用型硬件设计方案并自行研制开发了关键的硬件电路;在系统软件设计过程中采用面向对象设计思想,继承并封装了全部检测代码,根据测试需求分析的结果,修改、补充了新的属性和服务,增强了自动测试系统运行的稳定性和可靠性。     

Covariance Matrix for ?-?-? Filtering

Closed-form expressions are derived for the output noise response of an ?-?-? filter in steady-state operation with constant measurement noise statistics. To the author's knowledge such expressions have been unavailable until now. These formulas are useful for target tracking applications.     

高速干式加工技术

干式切削是指高速切削金属时不使用冷却液的一种加工方法。本文介绍了高速干式加工工艺、技术特点及发展趋势。     

Who is who in Algol-land ? - Part II -

In part I (De Greve and Packet) we have investigated the occurrence of reversed phases of mass-transfer during Case A evolution in close binaries. If the initial period of a system is shorter than 1–2 days (Early Case A) the reversed phase starts before core hydrogen exhaustion of the gainer (part I). This type of evolution is characterized by at least two phases of slow mass-transfer. We have computed the evolution of four Early Case A systems with initial masses of the loser equal to 3 Mo and 5 Mo. These four systems start mass-exchange when Xc of the primary has decreased to 0.525 (75% of its initial value). They all experience two phases of slow mass-transfer. We find that both phases have about the same duration for all systems. The mass ratios are clearly distinct, being closer to unity during the first phase. In the Hertzsprung-Russell, mass-radius and mass-luminosity diagrams both components remain close to the main-sequence band during slow mass-transfer. Evolution as an Algol is ended when both components overflow their outer critical surface after a second reversal of the mass-transfer. Observed Algol systems evolving in Early Case A are scarce. A search thruogh the catalogue by Giuricin et al. gives us the following candidates: X Tri, SX Aur and V Pup. Based on their mass ratios, SX Aur can tentatively be assigned to the first phase of slow mass transfer and X Tri to the second phase. For V Pup (which is more massive) this choice can not be made with certainty.     

Who is who in Algol-land ? - Part II -

In part I (De Greve and Packet) we have investigated the occurrence of reversed phases of mass-transfer during Case A evolution in close binaries. If the initial period of a system is shorter than 1–2 days (Early Case A) the reversed phase starts before core hydrogen exhaustion of the gainer (part I). This type of evolution is characterized by at least two phases of slow mass-transfer.We have computed the evolution of four Early Case A systems with initial masses of the loser equal to 3 Mo and 5 Mo. These four systems start mass-exchange when Xc of the primary has decreased to 0.525 (75% of its initial value). They all experience two phases of slow mass-transfer.We find that both phases have about the same duration for all systems. The mass ratios are clearly distinct, being closer to unity during the first phase. In the Hertzsprung-Russell, mass-radius and mass-luminosity diagrams both components remain close to the main-sequence band during slow mass-transfer. Evolution as an Algol is ended when both components overflow their outer critical surface after a second reversal of the mass-transfer.Observed Algol systems evolving in Early Case A are scarce. A search thruogh the catalogue by Giuricin et al. gives us the following candidates: X Tri, SX Aur and V Pup. Based on their mass ratios, SX Aur can tentatively be assigned to the first phase of slow mass transfer and X Tri to the second phase. For V Pup (which is more massive) this choice can not be made with certainty.     

Who is who in Algol-land ?- Part I -

We computed the evolution through case A mass transfer for 8 systems with mass of the primary equal to 3 and 5 M₀, mass ratios 0.7 and 0.9, and different periods. To this we added similar results from Packet (1988) for M_i = 9 M₀, q_i = 0.6, P_i = 1.62 d.During the mass transfer two competing mechanisms in the gainer decide on the evolution of the system: the rejuvenation of this star as the increasing convective core mixes fresh hydrogen into the inner regions, and the acceleration of nuclear burning, responding to the increasing mass.In all the cases the net result is a faster decrease of the central hydrogen content compared to the mass losing star. The secondary fills its own critical Roche lobe and reversed mass transfer starts.From our results and those of Nakamura and Nakamura (1984), we find that reversed mass transfer occurs after core hydrogen burning of the secondary (case A₁B₂) approximately for periods larger than 1 d (M_1i = 3 M₀) to 2 d (M_1i = 13.4 M₀). For smaller periods this happens before the gainer ends its core hydrogen burning (case A₁A₂).     

MJS-8型30秒计时器软件的设计

MJS-8型30秒计时器,采用8051单片机,利用可编程通用,键盘和显示器接口器件8279来完成整个系统。本文主要介绍软件部分的设计。