Application of artificial neural network to evaluation of dimensional accuracy of 3D-printed polylactic acid parts

Additive manufacturing (AM) has begun to replace traditional fabrication because of its advantages, such as easy manufacturing of parts with complex geometry, and mass production. The most important limitation of AM is that dimensional accuracy cannot be achieved in all parts. Dimensional accuracy is essential for high reliability, high performance, and useful final products. This study investigates the impact of printing parameters on the dimensional accuracy of samples fabricated through fused deposition modeling (FDM), an additive manufacturing (AM) method utilizing polylactic acid (PLA) material. The experimental design process was performed using Taguchi methodology. ANOVA was used to determine the most important parameter affecting accuracy. Based on experimental studies, the optimal printing parameters for parts are determined as follows: concentric infill pattern, 3 mm wall thickness, 70% infill density, and a layer thickness of 200 μm. Artificial neural network (ANN) was used in the evaluation and prediction of the results. The R-square (R²) performance evaluation criterion was above 95% from the ANN results. This value shows that the results are significant. The data acquired from this study may assist in identifying optimal parameters that contribute to the fabrication of samples with high dimensional accuracy using the FDM method.     

基于量纲分析和达西定律的地下化学爆炸气体泄漏规律

针对周围是均匀岩石介质的地下化学爆炸,研究爆炸后爆室内气体的泄漏规律.利用量纲分析,得到影响气体泄漏时间的主要物理量,包括气体动力学粘度、爆室内超压、围岩孔隙率及围岩厚度的平方与渗透率的比值等,并初步给出它们之间的函数关系.然后基于达西定律,推导计算气体泄漏时间的解析公式.得到的气体泄漏时间计算公式与通过量纲分析得到的定性函数关系式完全相符,二者从不同的角度对同一问题给出了相容的结果.可为地下化学爆炸气体泄漏的理论分析和规律性研究提供研究思路和工具,为地下爆炸有关的工程估算提供参考依据.     

A new three‐dimensional cobalt(II) coordination polymer based on V‐shaped 3,4′‐oxydibenzoate: synthesis,crystal structure and magnetic properties

A new coordination polymer (CP), namely poly[(μ‐4,4′‐bipyridine)(μ₃‐3,4′‐oxydibenzoato)cobalt(II)], [Co(C₁₄H₈O₅)(C₁₀H₈N₂)]_n or [Co(3,4′‐obb)(4,4′‐bipy)]_n ( 1 ), was prepared by the self‐assembly of Co(NO₃)₂·6H₂O with the rarely used 3,4′‐oxydibenzoic acid (3,4′‐obbH₂) ligand and 4,4′‐bipyridine (4,4′‐bipy) under solvothermal conditions, and has been structurally characterized by elemental analysis, IR spectroscopy, single‐crystal X‐ray crystallography and powder X‐ray diffraction (PXRD). Single‐crystal X‐ray diffraction reveals that each Co^II ion is six‐coordinated by four O atoms from three 3,4′‐obb^2? ligands, of which two function as monodentate ligands and the other as a bidentate ligand, and by two N atoms from bridging 4,4′‐bipy ligands, thereby forming a distorted octahedral CoN₂O₄ coordination geometry. Adjacent crystallographically equivalent Co^II ions are bridged by the O atoms of 3,4′‐obb^2? ligands, affording an eight‐membered Co₂O₄C₂ ring which is further extended into a two‐dimensional [Co(3,4′‐obb)]_n sheet along the ab plane via 3,4′‐obb^2? functioning as a bidentate bridging ligand. The planes are interlinked into a three‐dimensional [Co(3,4′‐obb)(4,4′‐bipy)]_n network by 4,4′‐bipy ligands acting as pillars along the c axis. Magnetic investigations on CP 1 disclose an antiferromagnetic coupling within the dimeric Co₂ unit and a metamagnetic behaviour at low temperature resulting from intermolecular π–π interactions between the parallel 4,4′‐bipy ligands.     

Symmetry Reductions,Group‐Invariant Solutions,and Conservation Laws of a (2+1)‐Dimensional Nonlinear Schrödinger Equation in a Heisenberg Ferromagnetic Spin Chain

Nonlinear spin excitations in ferromagnetic spin chains are studied for spintronic and magnetic devices including magnetic‐field sensors and for high‐density data storage. Here, (2+1)‐dimensional nonlinear Schrödinger equation is investigated, which describes the nonlinear spin dynamics for a Heisenberg ferromagnetic spin chain. Lie point symmetry generators and Lie symmetry groups of that equation are derived. Lie symmetry groups are related to the time, space, scale, rotation transformations, and Galilean boosts of that equation. Certain solutions, which are associated with the known solutions, are constructed. Based on the Lie symmetry generators, the reduced systems of such an equation are obtained. Based on the polynomial expansion and through one of the reduced systems, group‐invariant solutions are constructed. Soliton‐type group‐invariant solutions are graphically investigated and effects of the magnetic coupling coefficients, that is, α₁, α₂, α₃, and α₄, on the soliton's amplitude, width, and velocity are discussed. It is seen that α₁, α₂, α₃, and α₄ have no influence on the soliton's amplitude, but can affect the soliton's velocity and width. Lax pair and conservation laws of such an equation are derived.     

用于光催化领域的TiO_2与一维光量子阱复合结构的设计与优化

利用传输矩阵法设计并优化了用于光催化领域的TiO_2与一维光量子阱的复合结构,并分析了ZnS/SiO_2多层膜量子阱结构的透射特性.通过调节一系列的结构参数,在TiO_2光吸收波段(329.23 nm～482.71 nm)得到一个较宽的高反射率带隙,并且在吸收边附近(380 nm左右)得到了一个反射率高于93%的慢光子效应区.通过增加光线与TiO_2的作用时间和路径来提高光催化效率.     

拉曼光谱编码的荧光液相生物芯片检测系统研究

随着医疗诊断需求的增加,生物分子检测技术越来越受到人们的重视,液相生物芯片技术作为一种高通量,多通道的分子检测手段在近几年得到了飞速发展。通过层层自组装方法制备以微片为载体的拉曼光谱编码液相生物芯片,并利用自行搭建的一套高灵敏度、高分辨率的光学系统,实现对液相生物芯片的定性与定量分析。光学系统由拉曼光谱检测系统与荧光显微成像系统耦合而成。在拉曼光谱检测系统中激光器发射出785 nm波长的激光,通过二向色镜,带反反射镜与物镜汇聚到样品上,样品产生的拉曼散射光,经物镜,带反反射镜,二向色镜与拉曼滤波片,最后通过凹透镜聚焦到光谱仪的狭缝上,光谱仪色散实现在线阵CCD上拉曼光谱的获取。荧光显微成像系统应用光学成像原理,通过调节凹透镜与405 nm的激发光之间的距离,使激发光通过物镜均匀的照射到样品之上,样品激发出的荧光,通过物镜,带反反射镜,二向色镜,滤波片与相应的凹透镜,最后成像到面阵CCD上。改进传统便携式拉曼光谱检测系统光路并选用相应波段的带反反射镜与焦距20倍的物镜完成拉曼光谱检测系统与荧光显微成像系统的耦合。为了减少两路系统之间的相互影响选用合适的二向色镜以及滤波片,在提高耦合系统获取数据的准确性中有着重要的作用。该系统通过对反应之后的液相生物芯片进行拉曼光谱检测,以完成对每个编码玻片的定性识别,即解码;同时激发反应后液相生物芯片的荧光并采集荧光强度图,根据每个解码玻片上的荧光强度值完成对目标检测物的定量分析。区别于传统荧光编码液相生物芯片, 拉曼光谱编码具有稳定性更强,光谱分辨率更高等优点。该光学系统集拉曼光谱检测系统与荧光显微成像系统于一体,解决了目前未有基于拉曼编码的液相生物芯片的检测系统的问题,并且可同时对多种目标物进行识别和定量分析,提升了实验结果的准确性。     

中红外光谱结合向量夹角直接定量三氯蔗糖

多组分复杂体系的红外光谱由于成分多样、谱带严重重叠、背景干扰等导致谱图特征减弱,且体系中的红外光谱往往不是各组分光谱的简单叠加,需要借助于化学计量学技术以实现解析。基于朗伯-比尔定律（Lambert-Beer law）并且随着衰减全反射（ATR）技术取样普及,结合偏最小二乘回归法（PLS）、人工神经网络（artificial neural network, ANN）等化学计量法将数据进行累积、特征提取以及校正建模等工作解决红外光谱中严重重叠和非线性等问题,再采用二次测量定量分析已初步具有应用成效,而有效增强信息量表达,降低背景、噪声干扰,减少复杂的计算过程,进而保证定量分析结果的可靠性,则成为研究的主要方向。通过讨论光通道和背景对光谱强度变化的影响,结合向量角度转换提出一种新的近似线性定量方法。经初步理论计算,发现多组分混合物与该混合物中待测组分的相对含量二者间的向量夹角值存在一定的关系,而该关系并不受批次制样的影响,进一步通过高斯曲线模拟混合信号,充分说明选择合适的波长范围,二者在一定范围内存在线性相关性,相关性不受测量条件变化的影响。采用KBr压片法,向待测样品中逐步加入待测组分得到混合样本,分别得到待测组分光谱与混合样本光谱信号,先将其进行一阶求导,消除加性误差后,再将其转化为空间向量角度,消除批次制样中光程差异,再以百分比定义待测物样品的含量,所得到混合样的夹角值与其中所含参照品含量成简单线性关系,即以计算结果夹角值与含量作标准曲线,实现定量分析。本测量方法用于三氯蔗糖（Sucralose, TGS）与三氯蔗糖-6-乙酸酯（4,1,6-trichloro sucrose-6-acetate, TGS-6-A）二者进行一定比例混合（双组分体系）,以及TGS-6-A的脱酰产物（多组分体系）中的TGS的含量定量分析,在两种体系中定量均得到令人满意的结果,所建立标准曲线的相关系数r均达到0.995 0以上,相对误差均低于8.0%,所建立的分析方法对利用中红外透射光谱分析研究多组分样品具有重要的参考价值。     

金属切屑塑性流动的稳定性

对金属正交切削过程中切屑形成机制和材料塑性流动行为进行实验研究和理论分析. 通过对4 种常用金属材料正交切削过程的实验研究和切屑形貌的微观观察,确定了连续切屑转变成锯齿切屑的临界速度. 结果表明该临界速度与材料性能相关. 在实验观察基础上,提出描述材料正交切削过程的二维分析模型. 该模型假设切屑形成区为包括主剪切区和次剪切区的一个平行四边形. 载荷有主剪切区中的剪应力和次剪切区中的正压力;通过量纲分析得到描述材料正交切削过程的无量纲主控参数和无量纲形式的基本控制方程;应用线性稳定性分析方法建立平面应变状态下评价材料塑性流动稳定性的普遍准则;求得切屑形成区内材料塑性变形的速度和应力近似解. 讨论切屑形成、形貌转变以及相关的塑性失稳机制. 分析结果表明, 表征材料惯性与阻尼之比的无量纲参数— 雷诺数可以作为主控参数描述金属切削过程以及切屑材料塑性流动的稳定性.      

固体核磁共振定量表征方法及其在高分子结构研究中的应用

高分子材料拥有众多优良的特性,使其广泛应用于现代社会的生产、生活及高新科技等领域。对于高分子特性的研究离不开微观物理、化学结构的定量表征。在众多表征高分子结构定量信息的实验技术中,固体核磁共振（SSNMR）发挥着重要的作用。它可以定量表征高分子的化学结构、材料体系的相成分及共混组分等,从而实现了难溶高分子产物的结构鉴定,以及高分子微观物理、化学结构关联材料性能的研究。然而,传统的SSNMR定量方法（直接激发法,DD）往往需要耗费十几个小时甚至数天的实验时间。交叉极化方法（CP）虽然大大缩短了实验时间,却往往无法提供定量的信息。基于此,研究者们提出了多个定量CP的实验方法,同时满足了方法定量性和实验耗时短的需求。本文综述了传统SSNMR定量方法及几种定量的CP方法,简单介绍了每个方法的基本原理,并平行阐述了实验方法的应用范围及特点,通过部分实例展示了SSNMR定量方法在高分子材料领域的应用价值,为研究者研发新型的高分子材料提供可靠并有效的结构表征手段。