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     

主轴伸长量补偿在高速数控机床上的应用

文章设计并实现了高速数控机床主轴伸长量的实时补偿;分析了补偿的原理,提出了补偿的具体措施和实现方法,给出了补偿的PLC控制程序,并用一系列的试验数据证明了补偿的有效性。这种方法在实际机床应用中提高了机床的加工精度,具有广泛的推广价值。     

IP、ATM与MPLS技术特点分析研究

主要分析了IP、ATM以及MPLS技术的特点,对比了各自的优缺点,提出了所面对的困难,为今后的研究指出了方向.     

基于 FNN 机器人擦洗玻璃的力/位并环控制

对机器人的力反馈、主动柔顺控制和模糊神经网络进行了综合研究,提出了力/位并环控制策略,建立了相应的模糊神经网络结构,实施了力/位并环控制算法,在AdeptThree精密装配机器人进行了试验,取得了满意的效果。     

复合材料ENF试件裂纹扩展理论分析

对复合材料端部缺口弯曲（ENF）试件裂纹扩展过程进行了理论分析,研究了界面参数变化对载荷-位移曲线的影响。首先在梁微段分析的基础上,通过双线性Cohesive本构模型模拟了界面损伤。本文模型中考虑了轴力的影响,根据界面损伤程度对模型进行了分段,并分别获得了各段通解。以裂纹长度以及黏聚区范围为变量分析了ENF试件裂纹扩展过程,求解获得了载荷-位移曲线。通过与已有理论模型结果对比,验证了本文理论分析的正确性,且本文理论考虑了弹性段后非线性的存在。分析了界面参数与黏聚区长度的关系,为界面参数的选取提供了一定的依据。     

基于触发角定时控制的异步电机软起动控制器设计

针对起重设备专用三相异步电机的直接起动问题,分析了异步电机的T型等效电路,阐述了晶闸管调压电路的工作原理,提出了一种基于触发角定时控制的异步电机软起动方法。基于MATLAB/Simulink搭建了相应的系统仿真模型,进行了提出方法的仿真分析,验证了所提方法的正确性。最后,基于单片机设计了相应的软起动器的软硬件,进行了试验测试。结果表明提出的方法可以有效地实现三相异步电机的平滑起动,起动电流较小,有效地减少了起动过程对电机和电网的影响。     

复合材料 ENF 试件裂纹扩展理论分析简

 对复合材料端部缺口弯曲（ENF）试件裂纹扩展过程进行了理论分析,研究了界面参数变化对载荷-位移曲线的影响。首先在梁微段分析的基础上,通过双线性Cohesive本构模型模拟了界面损伤。本文模型中考虑了轴力的影响,根据界面损伤程度对模型进行了分段,并分别获得了各段通解。以裂纹长度以及黏聚区范围为变量分析了ENF试件裂纹扩展过程,求解获得了载荷-位移曲线。通过与已有理论模型结果对比,验证了本文理论分析的正确性,且本文理论考虑了弹性段后非线性的存在。分析了界面参数与黏聚区长度的关系,为界面参数的选取提供了一定的依据。     

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.     

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.     

中国航空发动机高压压气机发展的几个问题

叙述了全三维数值模拟技术的发展,分析了其局限性和解决途径;介绍了大小叶片设计技术的应用前景;探讨了提高高压压气机性能的技术途径;展望了中国高压压气机的发展;最后,给出了有益的启示。     

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 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。     

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.