高能CO2激光腔镜高反介质薄膜的传输特性

为了获得适用于高能CO2激光器的高抗破坏阈值高反薄膜,以10.6μm高反膜ZnSe/YbF3,PbTe/BaF2膜系为例,数值模拟了激光在高反介质膜中的传输的场特性;给出了激光在多层介质膜中的场强分布、温度场分布及热应力分布。结果表明硅镜基体上的PbTe/BaF2膜系所需膜层厚度小、膜层数少,反射率可高达99.98%。     

一种新的二维最大熵图象阈值分割方法

根据最大熵原理提出了一种用二维最大熵获取二值图象的新方法，介绍了用梯度－区域灰度均值二维最大熵求取阈值的原理和过程。计算机仿真结果表明，采用本文提出的阈值分割方法，对于直方图平坦的灰度图象处理效果尤为理想。     

测量透明位相物场的激光纹影-散斑干涉系统(英文)

本文给出了诊断相位场,如燃烧、对流、自由射流、超声速流场和等离子体等的一种激光纹影-散斑干涉系统。利用这套光学系统可在同一瞬时获得流场的散斑图和与之相应的剪切干涉图。作为实验,对一非定常波动的火焰(本生灯)进行了测试,实验表明用散斑照相术有可能得到密度波动的湍流场的定量结果;作为定量测试,对一沿竖直平板的自然对流,同时应用散斑照相和差纹影干涉术进行了定量分析,其结果的一致性很好。本文最后给出了散斑图的傅氏变换空间滤波的全场类似子纹影干涉图的流场显示照片。     

基于最小一乘的跑道入口高度计算

跑道入口高度是关系着飞机能否安全着陆的关键参数,在其计算中需要采用曲线拟合预测的方法。目前大多是采用基于最小二乘准则的拟合方式。由于最小二乘准则的局限性,当下滑道随机误差不满足正态分布,在飞行数据中出现异常点时会给预测带来较大误差。将最小一乘方法引入到跑道入口高度计算问题中,提高了算法的稳健性,很好地克服了这一问题。     

Microstructure,porosity and mechanical properties of selective laser melted AlSi10Mg

Finite element modeling (FEM), microscopy, X-ray computed tomography (CT) and mechanical property tests were used to study the microstructure, porosity and mechanical properties of an AlSi10Mg alloy produced by selective laser melting (SLM). The simulation of the melt pool and thermal history under different energy densities produced an optimized result with an energy density of 44.5 J·mm⁻³. The high cooling rate during the SLM process significantly refined the previous α-Al dendrites. The growth direction of the network-like Al-Si eutectic structure at different orientations confirmed the anisotropic nature of the microstructure. Furthermore, the microhardness, tensile testing and fracture analysis results proved that there were no obvious distinctions in the strength between the transverse and longitudinal directions, and that the ductility was anisotropic, possibly due to the shape and distribution of the pores. The pores measured by X-ray CT at different energy densities confirmed that the sphericity of the pores was inversely related to pores volumes. With optimized processing conditions, the porosity of the selective laser melted sample decreased leading to the improved fabricated fuel system component via SLM.     

空间激光通信系统中的信道纠错编码技术

由于空间激光通信系统的信道状态和链路捕获跟踪的不确定性,多种形式的信道纠错编码技术正被广泛发展研究。结合空间激光通信链路中误码性能的主要影响因素,分别选择合适的编码方案进行分析。通过仿真实验可知,对于在大气结构参数为1.5×10~(-14) m~(-2/3)、风速为20 m/s的空地激光链路的环境下,在系统数据速率为2 Gbit/s、要求误码率为10~(-6)时,LDPC码结合交织码相对未编码系统有3 dB的等效编码增益,LT码相对未编码系统有3.8 dB的等效编码增益。提供了一种能快速生成、扩展和校验的编码和交织实现方法,以抵抗大气湍流的快速变化对系统性能产生的影响。     

基于PAM-CRASH的蒙皮典型结构高速冲击仿真

以典型蒙皮结构为研究对象，分别对由2024－T3铝合金和碳纤维复合材料交替层压而成的FMLs以及2024－T3铝合金蒙皮进行高速冲击有限元仿真，并进行了损伤对比。其中，铝合金层和碳纤维层均采用最大应变准则。利用碰撞模拟分析软件PAM-CRASH以及采用SPH弹体对冲击模型进行仿真，结果显示在相同冲击能量下，加了支承结构的蒙皮在损伤抗性方面有了明显提升，并在此基础上分析不同的纤维铺层角度和铺层方式对FMLs蒙皮性能的影响。     

基于激光的便携式飞机装配接缝质量检测仪及应用

介绍了一种基于激光的便携式接缝质量检测仪的工作原理及硬件组成。使用该检测仪对飞机缝隙和台阶阶差进行了测量,通过与人工测量进行对比验证,证明了该装置可实现对特征三维信息的快速自动检测,工作准确可靠。     

A shortcut to marking 3D target curves on curved surface via a galvanometric laser scanner

Marking arbitrary three-dimensional(3D) target curves on given objects with curved surface is required in many industrial fields, such as fabric prepreg placement in composite material part fabrication, product assembly, surface painting for decoration, etc. A shortcut to the solution of this intractable problem is proposed by utilizing a galvanometric laser scanner(GLS) with the aid of a camera. Without using the existing tedious GLS calibration procedures,the proposed method directly establishes a mapping between the 3D coordinates of the laser spots on the object surface and the control voltages of the scanner. A single-hidden layer feedforward neural network(SLFN) is employed to model the mapping. By projecting a dense grid of laser spots on the object to be marked and simultaneously taking only one image, the SLFN model is trained in minutes via a linear solving mechanism. Experiments demonstrate that the trained SLFN model has a good generalization performance for marking 3D target curves. The 3D laser marking errors on experimental objects are less than 0.5 mm. The proposed method is especially suitable for on-site use and can be conveniently extended to multiple GLSs for marking large complex objects.