基于相空间重构的f_0F_2一步预测算法研究

利用低纬度地区某垂测站2005年3月和4月两个月,f0F2参数共5856个数据样奉,对提前15min的一步预测算法进行了研究.基于混沌时间序列的相空间重构方法,以相近邻点轨迹具有相似性为预测理论基础,采用k最近邻点的方法对下一时刻的,f0F2进行预测.对邻点个数的选取采用了训练法和自适应选择法,对选出的邻点采用平均法和自回归两种方法进行处理,并对几种不同方法的预测结果进行了比较.结果证明,基于相空间重构的一步预测算法预测精度较高,并且容易实现,运算速度高,适用于电离层参数准实时预报.     

S06钢疲劳性能及其概率特性

采用高频疲劳试验方法对新型高强度沉淀硬化马氏体不锈钢S06钢中长寿命疲劳性能进行了测量,结果发现:随着应力水平降低,疲劳裂纹趋向于从试样内部萌生,裂纹内部萌生的试样寿命高于表面萌生的试样寿命,二者分散性很大.为了对S06钢长寿命疲劳数据概率特性进行正确的评估,主要对内部萌生机制下的数据进行了研究:利用定时截尾数据的极大似然估计方法和定时截尾数据的柯尔莫哥洛夫检验方法对长寿命区一定应力水平下的疲劳寿命概率分布情况进行了研究,结果表明疲劳寿命服从对数正态分布;采用考虑越出数据的极大似然方法对S06钢应力寿命数据进行拟合,建立了P-S-N曲线模型;利用P-S-N曲线对S06钢长寿命区疲劳强度概率分布进行了讨论.     

电离层F层中舒曼共振现象的检测

利用Ａｕｒｅｏｌ－３卫星在电离层Ｆ层高度上（６５０ｋｍ左右）对电离层电场扰动与电子密度扰动的观测进行分析处理,在高纬电离层Ｆ层高度上可以检测到舒曼共振现象。根据等离子体参数,可以认为,发生在这个高度上的舒曼共振现象与Ｌ模式的波传播有关,舒曼共振的基频是与电子密度的大尺度不规则性有关,谐波分量与正向密度梯度相关。     

从F100看战斗机发动机研制思想的进步

自20世纪60年代后期,F100发动机经历了方案论证、型号研制、初期使用、耐久性提高、改进改型、使用保障等阶段,目前仍是第3代前线战斗机F-15和F-16的主要动力装置.通过F100发动机的研制历程,可以发现无论是F100发动机性能极大提高与改进改型成功的经验,还是F100发动机使用初期故障频发、与空军出现争议、转入生产遇到困难、批量使用故障时发等,都值得总结和借鉴.     

表面钝化对超临界航空煤油静态结焦特性影响

通过静态装置,研究了不锈钢经表面磷化、酸洗钝化以及电解钝化后对超临界压力下航空煤油RP-3热氧化结焦的抑制效果,并对表面钝化层的耐久性做出评估.研究发现,不锈钢的钝化膜层有效地降低不锈钢表面催化活性,按结焦抑制效果排序为:电解钝化>酸洗钝化>磷化;化学稳定性好、耐蚀性强的钝化膜层会延长材料的使用寿命,按钝化膜耐蚀性排序为:电解钝化>酸洗钝化>磷化;综合结焦抑制效果及化学稳定性两个因素考虑,电解钝化为最佳表面钝化方案,但其在高温高腐蚀的煤油环境下长时间实验时易失去钝化效用.     

F1方程式赛车后升力翼的气动特性

以比例为1∶3的F1方程式赛车后升力翼为研究对象,研究了后升力翼攻角变化对F1方程式赛车气动阻力和气动升力的影响规律.在攻角为12°时,气动升力与气动阻力的比值的绝对值达到最大,此攻角就是F1方程式赛车后升力翼的最佳攻角,模型风洞试验验证了这一结论.      

释放SF_6气体改变电离层电子密度的实验研究

电离层受到自然或人工扰动后产生的电子密度变化会影响无线电的传播。实验模拟了人工释放SF_6气体扰动电离层,通过对SF_6气体在电离层中的扩散过程和相应的离子化学反应的分析,并结合实验测量,研究了电离层电子密度随SF_6气体释放量的变化规律。实验结果表明:SF_6气体在电离层高度释放后,电子密度显著减少,且减少量与气体释放量在一定范围内呈负指数关系。研究可为今后提高卫星通信保密性和实施通信干扰等应用提供理论依据。     

Influence of laser shock peening on surface integrity and tensile property of high strength low alloy steel

Laser Shock Peening (LSP) is a well-established surface treatment commonly used to improve mechanical properties of material's surfaces. To further understand the relationship between tensile property and fatigue life improvement of high strength low alloy steel in the LSP process, LSP treatment of 32CrNi high strength low alloy steel was carried out by YAG laser with pulse energy of 15 J, and tensile property was tested by electronic universal material testing machine. Surface morphology, residual stress and tensile fracture of the specimens before and after LSP were observed by white light interferometer (WLI), X-ray measuring apparatus and scanning electron microscope (SEM). Result shows that LSP did not change tensile strength of 32CrNi steel but cause yield characteristic transform from obvious yield point to no yield phenomenon which is the only factor benefiting fatigue life, indicating that the increment of fatigue life was probably related to the disappearance of yield phenomenon. Formation mechanisms of tensile fractures and yield phenomenon induced by LSP at room temperature were also discussed and completely revealed. Deeper compressive residual stress and flat grains contributed to the transition of yield characteristic and lower elongation rate of 32CrNi steel subjected to LSP.     

In-situ observation and finite element analysis of fretting fatigue crack propagation behavior in 1045 steel

In this paper fretting fatigue crack behavior in 1045 steel is studied by in-situ observation and finite element analysis. in-situ fretting fatigue experiments are conducted to capture real-time fretting fatigue crack formation and propagation process. The fretting fatigue tests under different load conditions are carried out, then the lifetime and fracture surface are obtained. The crack propagation rates under different loading conditions are measured by in-situ observations. With in-situ observation, crack initiation location and direction are analyzed. Finite element model is used to calculate J-integral which then is applied to fitting with experimental crack growth rate, and establishing crack growth rate model. From fitted S-N curve, it turns out that smaller load ratio leads to higher lifetime. Crack initiates slightly below the point equivalent to line contact of the contact surface in different test conditions, and crack direction shows no obvious relationship with load parameters. The established crack growth rate model well agrees with the test results.