柱形等离子体辐射场的数值计算和分析

参照金属辐射场的求解方法,在简化条件下计算出柱形等离子体行波传输和驻波传输的辐射图．当改变等离子体密度以及相关参数时,对应的辐射图会相应地发生变化,得出与信号在金属介质中传输相类似的结果．根据理想柱形等离子体表面波的色散关系得到波矢,求出的柱形等离子体辐射方向图与金属介质的辐射方向图相比,会发生较大的变化,因此利用等离子体进行信号传输有一定的价值．     

参量激励过程中三波耦合的一般色散关系(Ⅱ)一般色散关系以及泵场阈值和增长率

本文讨论了各向同性的均匀有耗电离层背景下激励参量不稳定性的三波耦合过程．首先推导有耗情况下参量激励过程中的一般色散关系,然后针对文献得出的两种频率和波矢匹配条件计算激励参量不稳定性所需要的泵波阈值场强和受激励的等离子体波的增长率．结果表明,过密加热时泵场阈值与电子碰撞频率和离子碰撞频率的乘积成正比,不同于以前的一些理论模型得到的泵场阈值与碰撞频率的一次方成正比的结论;欠密加热比过密加热需要能量更高的高频泵波来激励参量不稳定性．     

碳纤维增强点阵夹芯结构的散热承载协同优化

在散热性能分析中,解析地给出了点阵夹芯结构的整体传热系数和等效压降,定义了散热性能指标.通过连续介质力学的方法和经典的层合理论,并通过串并联模型给出了碳纤维增强点阵夹芯结构整体的刚度特性.在满足既定的承载要求和一定的散热要求约束下,提出了一种对碳纤维增强点阵夹芯结构进行多功能优化设计的协同优化方法,在设计中采用了更符合工程实际的基于分枝定界法的混合离散优化方法,得到了夹芯结构质量函数的最小值,从而实现了轻质的目的.同时对不同结构形式的芯子做了相应的比较和分析,结果表明:金字塔型点阵夹芯结构在实现轻质的同时,具有较强的散热能力,而且承载能力更好,更为轻质高效.      

功率组件基于等离子清洗的免钎剂真空软钎焊技术

为解决功率电子产品中陶瓷电路板与热沉载体功率组件焊接效率低、空洞率高等问题,对焊接过程中的焊料类型,真空度以及空洞率进行了研究,提出了一种新的免钎剂真空焊接方法。研究结果表明,使用等离子清洗的焊片可显著提高抽真空速率,并减少气泡,降低空洞率;采用新焊接方法得到的试样空洞率低、焊接效率高、质量一致性好,可用于高可靠性功率电子产品中。     

力限振动试验条件设计方法

给出了一种基于复杂二自由度模型的力限振动试验条件设计方法.该方法应用动态子结构法计算试验件结构和支持结构的模态有效质量和剩余质量,根据模态有效质量在频域上的分布情况确定不同频带内振动系统的复杂二自由度模型参数,结合支持结构激励条件给出试验件与支持结构接触面的力谱和加速度谱,在此基础上进行包络,得到力限振动试验剖面.仿真结果表明,由该方法给出的力限振动试验条件,与传统加速度试验条件相比,能更加真实地反应试验件的振动环境.      

等离子体诊断中扫描电压源的研制

详细叙述了扫描电压源的硬件和软件组成,并通过采用PCI-6251数据采集卡、PA93功率放大电路和虚拟仪器软件LabVIEW及工控机相结合, 突破了关键技术,成功研制了一套扫描电压源并应用于等离子体诊断,使整个测试过程非常快, 可以在秒级的时间内完成, 相对于手动测试,该实验得到的数据更为精确, 实时获得了等离子体的伏安(I-V)特性曲线和数据处理结果。     

L、S频段电磁波在等离子体中衰减实验研究

利用低气压辉光放电原理在地面产生大面积、长时间稳定持续的可控等离子体,在此基础上进行了L、S频段的电波传播衰减实验,在实验室环境下持续再现了“黑障”现象,并获得了1.57GHz和2.49GHz电磁波衰减量随等离子电子密度变化的规律。将实验数据与经典传播理论以及薄层理论的预期值对比,结果表明：电波的衰减趋势与经典理论预期基本相符,验证了本文所提出的新实验方法的有效性;在等离子厚度约为波长的1倍与1.5倍条件下,未观测到明显的薄层效应。     

Numerical research on airfoil transition delay by alternative current dielectric barrier discharge actuation

A Dielectric Barrier Discharge (DBD) plasma actuator can create a body force which locally accelerates the base flow leading to an attenuation of broadband disturbance to delay the transition. In this study, numerical simulation on an NLF0416 airfoil is conducted to investigate transition delay and drag reduction by a DBD plasma actuator. To simulate plasma’s effect more accurately, boundary-layer data is acquired from Reynolds Averaged Navier Stocks (RANS) equations instead of laminar boundary layer equations, although RANS equations need a much finer boundary-layer grid, and the linear stability analysis method is used to analyze the boundary layer and get the transition point. In this study, the influences of different actuation intensities and positions are investigated, and results show that if the actuation intensity is stronger and the actuation position is closer to the base transition point, more drag reduction can be obtained. However, the efficiency of plasma transition delay is really low. For example, when the actuation voltage is 16 kV, the actuation frequency is 1 kHz, and the main Mach number is 0.1, the saved power due to drag reduction is about 5.09 W, but the power consumed is about 32.61 W, and the efficiency is just 15.6%.     

双层旋转锥形液膜一次破碎特性数值研究

为了全面加深对锥形液膜一次破碎机理的认识,对双层锥形液膜的雾化过程进行了数值模拟,重点研究了压降和同轴旋转空气对双层液膜宏观形态、液膜破碎模式、液膜破碎长度和喷雾锥角等液膜一次破碎特性的影响。数值计算的喷雾场宏观形态与试验结果接近,喷雾锥角和索特尔平均直径的计算最大误差分别为4.9%、7.4%。研究表明：同轴旋转空气参与雾化会改变喷雾场的整体形态;增大压降和空气速度会改变液膜的破碎模式和主导表面波模式;双层液膜的合并会在液膜表面产生剧烈的表面波动,同时会略微增大液膜的喷雾锥角;液膜的破碎长度会随着压降和同轴旋转空气轴向速度的增大而减小。该研究有助于进一步研究双层液膜一次破碎的机理,从而指导对双路离心式喷嘴的雾化认识。     

Confinement characteristic of primary electrons with the variation of channel width in the discharge chamber of annular ion thruster

In this paper, the confinement characteristic of primary electrons in the non-axisymmetric discharge chamber of annular ion thruster is investigated by a three-dimensional (3D) non-self-consistent particle tracking model with Monte Carlo Collision (MCC) method. The results show that: The density of primary electrons upstream of ion optics on cathode axis is about 5–50 times higher than that of the other side, which means that the density of primary electrons is obviously non-axisymmetric. The channel width has a significant effect on the average density and uniformity of primary electrons. The average density can be increased by nearly 1.5 times under the appropriate channel width, meanwhile, the variance of density distribution can be reduced by more than 2 times. This is because that increasing the channel width can improve the average confinement length of primary electrons greatly. Furthermore, there is an infection point in the increase of primary electron average confinement length with the channel width, which caused by the significant change of magnetic field structure. Under the case after the inflection point, primary electron mainly (more than 50%) moves to the channel center, which makes the average confinement length of primary electrons and their number in the discharge chamber increase largely.