截幅效应对DMT调制的影响及一种减小截幅噪声的方法

ＤＭＴ（ＤｉｓｃｒｅｔｅＭｕｌｔｉｔｏｎｅ）调制是一种在ＡＤＳＬ（ＡｓｙｍｍｅｔｒｉｃａｌＤｉｇｉｔａｌＳｕｂｓｃｒｉｂｅＬｉｎｅ）中被广泛采用调制技术。本文分析了在ＤＭＴ中对信号进行截幅所产生的影响，计算了Ｄ／Ａ变换产生的量化噪声和截幅噪声，并与未截幅时相比较，在不降低ＳＮＲ的情况下，降低了Ｄ／Ａ变换器的精度的要求，并求出最佳截幅因子。本文分析了一种减小截幅噪声的方法，并说明在非最佳截幅时，通过这种方法可获得与最佳截幅同样的结果。     

用解冻焦散线法测定平面应变裂纹的应力强度因子K_Ⅱ

本文就奇异点附近的变形可表示为一维函数的情况,导出了奇异点附近变形的凸凹性对照射光源的要求。用焦散线的这种性质测定平面裂纹的应力强度因子ＫⅡ,收到意想不到的效果。     

边界元法在薄壁杆扭转问题中的应用

本文运用边界元法,分析研究了角形和箱形这类截面薄壁杆在扭转时的剪应力分布规律及应力集中问题.     

基于燃油压力波的柴油机高压喷射系故障信息的研究

本文从柴油机燃油压力波的特征出发,建立ARI(Auto—Regressive Integra—ted)时序参数模型.通过对不同故障下的燃油压力波基于ARI时序参数的现代谱分析,说明ARI时序参数模型较好地揭示了燃油压力波蕴含的故障信息.通过燃油压力波的ARI时序参数构造故障诊断模式向量,根据几何距离与信息距离的测度来诊断故障,具有一定的实践意义.     

关于潜艇装备劳兰C导航仪技术问题的研究

本文提出了一种改善潜艇现有天线接收性能的方法,从而解决了在潜艇上安装使用劳兰C导航仪的关键技术问题。     

爆轰波在可压缩金属板面上斜反射初始参数的计算

本文计算了爆轰波在可压缩金属板面上斜反射时的初始参数。计算中选用的五种炸药是TNT(p_0为1.64g/cm~3,1.45g/cm~3)、RDX(p_0为1.59g/cm~3,1.76g/cm~3,1.80g/cm~3)、RDX/TNT(77/23)(p_0为1.75g/cm~3)、Pentolite(p_0为1.65g/cm~3,1.68g/cm~3)和B 炸药(p_0为1.71g/cm~3);三种介质是铁、铜和铝。     

921A钢动态屈服应力的实验研究

本文采用较为先进的实验技术——高应变率下材料的分段式Hopkinson拉杆实验(分段式—维杆拉伸实验)研究了“921A”钢在高应变速率情况下的动态屈服性能,获得了很有理论和实用价值的应变率ε—功屈服应力σ_d变化曲线。同时本文简要介绍了分段式Hopkinson拉杆实验技术的基本原理和实验方法。     

固体热容激光器温度场应力场分析

采用有限元分析方法,对Nd:YAG作为激活介质的固体热容激光器的温度场及应力场进行了研究.结果表明固体热容激光器的温度场、应力场与常规的固体激光器有很大的差异,常规的固体激光器激活介质必须在泵浦的同时进行冷却,晶体表面温度比中心温度低,晶体表面受到的是张应力.固体热容激光器发射激光时,激活介质处于绝热状态.激活介质表面的温度要比中心高,激活介质表面出现的是压应力.这种差异是固体热容激光器可以高功率运转的物理机制.     

Numerical simulation of the blast wave of a multilayer composite charge

The numerical simulation of a blast wave of a multilayer composite charge is investigated. A calculation model of the near-field explosion and far-field propagation of the shock wave of a composite charge is established using the AUTODYN finite element program. Results of the near-field and far-field calculations of the shock wave respectively converge at cell sizes of 0.25–0.5 cm and 1–3 cm. The Euler––flux-corrected transport solver is found to be suitable for the far-field calculation after mapping. A numerical simulation is conducted to study the formation, propagation, and interaction of the shock wave of the composite charge for different initiation modes. It is found that the initiation mode obviously affects the shock-wave waveform and pressure distribution of the composite charge. Additionally, it is found that the area of the overpressure distribution is greatest for internal and external simultaneous initiation, and the peak pressure of the shock wave exponentially decays, fitting the calculation formula of the peak overpressure attenuation under different initiation modes, which is obtained and verified by experiment. The difference between numerical and experimental results is less than 10%, and the peak overpressure of both internal and external initiation is 56.12% higher than that of central single-point initiation.     

Experimental research on the instability propagation characteristics of liquid kerosene rotating detonation wave

In order to study the instability propagation characteristics of the liquid kerosene rotating detonation wave (RDW), a series of experimental tests were carried out on the rotating detonation combustor (RDC) with air-heater. The fuel and oxidizer are room-temperature liquid kerosene and preheated oxygen-enriched air, respectively. The experimental tests keep the equivalence ratio of 0.81 and the oxygen mass fraction of 35% unchanged, and the total mass flow rate is maintained at about 1000 g/s, changing the total temperature of the oxygen-enriched air from 620 K to 860 K. Three different types of instability were observed in the experiments: temporal and spatial instability, mode transition and re-initiation. The interaction between RDW and supply plenum may be the main reason for the fluctuations of detonation wave velocity and pressure peaks with time. Moreover, the inconsistent mixing of fuel and oxidizer at different circumferential positions is related to RDW oscillate spatially. The phenomenon of single-double-single wave transition is analyzed. During the transition, the initial RDW weakens until disappears, and the compression wave strengthens until it becomes a new RDW and propagates steadily. The increased deflagration between the detonation products and the fresh gas layer caused by excessively high temperature is one of the reasons for the RDC quenching and re-initiation.