低速气流三参数动态测量软件初探

本文采用虚拟仪器概念和技术,构建了三孔探针动态测量系统。该系统集成了高速数据采集、储存及现代数据处理模块,通过该系统可动态显示低马赫数下压气机内部流场的总压、静压、速度矢量等物理参数的变化趋势,并可对动态信号进行时域显示和频域分析。系统还具备自动标定、零漂消除及线性度拟合的功能,实现了流场动态测试技术在线处理与测试同步进行的目的。     

H_2BPMPBD和DAM协同萃取部分Ln(Ⅲ)

4 酰代双吡唑啉酮是以吡唑酮为端基、脂肪族碳氢取代基联结而成的一类新型非环四齿酸性螯合剂[1 ,2 ] ,螯合功能团比普通的 4 酰代吡唑酮多一倍 ,对金属离子具有很强的萃取能力 ,其中对Ｆｅ(Ⅲ )、Ｃｏ(Ⅱ )、Ｎｉ(Ⅱ )、稀土离子的萃取分离以及稀土荧光配合物方面的研究已有报道[3～ 5] 。为了进一步探讨该类萃取剂的萃取性能 ,在合成萃取剂 1 ,4 双 ( 1′ 苯基 3′ 甲基 5′ 氧代吡唑 4′ 基 )丁二酮 [1 ,4]的基础上 ,研究了Ｈ2 Ａ与ＤＡＭ的氯仿溶液从硝酸介质中协同萃取Ｌｎ(Ⅲ )的性能。通过考察萃取剂浓度和溶液酸度等因素对Ｌｎ(Ⅲ …     

固相萃取/超高效液相色谱-串联质谱法测定儿童化妆品中新康唑等4种抗生素

建立了测定儿童化妆品中新康唑等4种抗生素的超高效液相色谱-串联质谱法(UPLC-MS/MS)。样品经70%乙腈水溶液超声提取后,使用SCX固相萃取小柱净化,以0.1%甲酸水和乙腈作为流动相,经Waters ACQUITY BEH C₁₈(2.1 mm×100 mm,2.5μm)色谱柱分离,使用多反应监测模式(MRM)进行测定。结果表明,4种抗生素线性关系良好,相关系数(r)均为0.999,方法检出限(LOD)和定量下限(LOQ)分别为0.005～0.250μg/g和0.010～0.500μg/g。4种抗生素在3种基质和3个加标水平的平均回收率为89.3%～113%,相对标准偏差(RSD)为0.90%～7.2%。该方法高效、准确、特异性好,满足新康唑等4种抗生素在儿童化妆品中的测定需求。     

Ru掺杂对Fe催化剂上酚类化合物加氢脱氧影响的密度泛函理论研究北大核心CSCD

采用密度泛函理论(DFT)计算研究了苯酚、邻甲酚、愈创木酚在不同结构Ru-Fe(211)表面上吸附活化性能和加氢脱氧反应路径.结果表明,Ru掺杂能促进H2分子在Fe(211)表面上解离,提高加氢脱氧反应速率.酚类在1Ru_(ads)-Fe(211)表面上吸附比在1Ru_(sub)-Fe(211)表面上更稳定,苯酚和邻甲酚脱羟基步骤能垒分别降低0.13和0.28 eV,有利于生成芳烃.愈创木酚在1Ru_(sub)-Fe(211)表面上加氢脱氧优势路径是先脱甲氧基生成苯酚,苯酚再加氢脱氧生成产物苯(速控步骤能垒1.16 eV);而在1Ru_(ads)-Fe(211)表面上愈创木酚先脱羟基再脱甲基生成苯酚的路径更具有动力学优势(速控步骤能垒1.21 eV).计算结果表明Ru掺杂方式影响Fe催化剂对酚反应分子的吸附稳定性以及加氢脱氧反应路径和性能.与1Ru掺杂Fe(211)催化剂相比,增加Ru原子数形成4Ru_(ads)-Fe(211),能够进一步提高酚类反应物的吸附强度,但导致加氢脱氧反应能垒升高.因此,在Fe催化剂上以表面吸附的形式掺杂少量贵金属Ru更利于酚类加氢脱氧生成芳烃.     

两个含5-溴水杨酸钠(Ⅰ)/镉(Ⅱ)配合物的合成、晶体结构、Hirshfeld表面分析与抑菌活性

由 5-溴水杨酸(H₂BB A)合成了钠(Ⅰ)/镉(Ⅱ)配合物[Na(HBBA)]_n (1)和[Cd(HBBA)₂(4,4′-Bipy)]_n (2)(H₂BB A=5-溴水杨酸,4,4′-Bipy=4,4′-联吡啶)。通过元素分析、红外光谱、热重、粉末X射线衍射和单晶X射线衍射表征了其结构。配合物1的不对称单元中有1个钠离子和1个HBBA^-。钠离子是六配位的三棱柱构型,HBBA^-配体的3个氧原子分别与2个钠离子配位,连接相邻的钠离子形成了3条一维链结构,HBBA^-配体连接相邻的3条一维链形成了二维网络结构。分子间氢键连接相邻的二维网络结构形成了三维氢键网络结构。配合物2中有1个镉离子、2个HBBA^-和1个4,4′-Bipy。镉离子是六配位的扭曲八面体构型,4,4′-Bipy配体连接相邻的2个镉离子形成了一维链结构。分子间氢键连接相邻的一维链结构形成了三维氢键网络结构。通过Hirshfeld表面和指纹图分析了配合物晶体中的弱分子间作用力。详细研究了配合物1和2的热稳定性和抑菌活性。     

几种改进的CoMFA方法比较研究血小板活化因子拮抗剂

由于传统的比较分子场分析(CoMFA)方法本身存在一些缺陷，使得分子的叠合 规则以及叠合分子的空间取向和空间位置等因素对q~2的影响很大，因此相继提出 了几种改进的CoMFA方法。为了优化CoMFA结果，应用传统的CoMFA方法和交叉验证 的R~2引导的区域选择法(q~2-GRS)、全取向搜索法（AOS）、全空间搜索法（APS） 以及比较分子相似性指数(CoMSIA)等四种改进的CoMFA方法，对18个pinusolide类 衍生物这类新发现的血小板活化因子（PAF）拮抗剂进行了比较研究。结果表明四 种改进的CoMFA方法得到的q~2值均比传统CoMFA的高。q~2-GRS方法得到的q~2值有 所提高，但综合结果并不理想，AOS与APS得到的q~2较为理想，而在CoMSIA中， q~2几乎不受空间取向或空间位置的影响。同时我们引人基于样本的偏最小二乘法 （SAMPLS）取代原AOS／APS程序中的传统PLS进行统计分析，明显提高了其运行速 度。最后，根据q~2最高的CoMFA模型和CoMSIA模型设计了几个预测活性更高的 pinusolide类似物。     

二维铁电材料ABP2X6内在极高的负泊松比

Recently, ferroelectric materials have attracted considerable research attention. In particular, two dimensional (2D) ferroelectric materials have been considered as most crucial for next-generation circuit designs because of their application as novel electric memory devices. However, a 2D ferroelectric material is very rare. The ferroelectric materials with the form ABP₂X₆ (A = Ag, Cu; B = Bi, In; X = S, Se) are of interest because of their ferroelectric property maintained in their ultrathin structures. Within the ABP₂X₆ monolayer, the P―P bonds form the pillars that hold the top and bottom X planes, while the off-center A―B atoms between the X layers induce a spontaneous ferroelectric polarization. If the two off-center A―B sites are equally aligned, this would lead to the appearance of the paraelectric state. Such intriguing structures must impart novel mechanical properties to the materials. Until now, there has been no report on the mechanical properties of monolayer ABP₂X₆. Based on first-principles calculations, we studied the structural, electronic, mechanical as well as the electromechanical coupling properties of monolayer ABP₂X₆ (A = Ag, Cu; B = Bi, In; X = S, Se). We found that they are all semiconductors with wide bandgaps of 2.73, 2.17, 3.00, and 2.31 eV for CuInP₂Se₆, CuBiP₂Se₆, AgBiP₂S₆, and AgBiP₂Se₆, respectively, which are calculated based on the Heyd-Scuseria-Ernzerhof (HSE) exchange correlation functional model. The conduction band minimum is mainly from p orbitals of X and B atoms, whereas the valence band maximum is due to the hybridization of the p orbital of X atoms and the d orbital of A atoms. Moreover, there are three short and three long A/B―X bonds due to the A―B off-center displacement. Together with the d-p orbital hybridization, the main reason for the distorted ferroelectric structure in ABP₂X₆ monolayers is the Jahn-Teller effect. ABP₂X₆ monolayers are predicted to be a new class of auxetic materials with an out-of-plane negative Poisson's ratio, i.e., the values of the negative Poisson's ratio are in the order AgBiP₂S₆ (−0.805) < AgBiP₂Se₆ (−0.778) < CuBiP₂Se₆ (−0.670) < CuInP₂S₆ (−0.060). This is mainly due to the tensile strain applied in the x/y direction enlarging the angle between P―P bonds and top layer X atoms, thereby enhancing the bucking height of monolayer ABP₂X₆. Moreover, external strain has a significant impact on the A―B off-center displacement, rendering an out-of-plane piezoelectric polarization. The values of e₁₃ for CuInP₂S₆, CuBiP₂Se₆, AgBiP₂S₆, AgBiP₂Se₆ monolayers are calculated to be −3.95 × 10⁻¹², −5.68 × 10⁻¹², −3.94 × 10⁻¹², −2.71 × 10⁻¹² C∙m⁻¹, respectively, which are comparable to the only experimentally confirmed 2D out-of-plane piezoelectric Janus system (piezoelectric coefficient = −3.8 × 10⁻¹² C∙m⁻¹). This unusual auxetic behavior, ferroelectric polarization, and the electromechanical coupling in monolayer ABP₂X₆ could potentially lead to enormous technologically important applications in nanoelectronics, nanomechanics, and piezoelectrics.     

An Oscillation Condition for an Electrode－separated Piezoelectric Sensor in Non－electrolyte Liquid

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Time-Resolved Photoluminescence Spectra of Porous Si

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