直流电弧等离子体炬的特性研究

介绍了局部热力学平衡下描述直流电弧等离子体炬的磁流体力学模型，采用数值模拟方法研 究了等离子体炬内等离子体的传热和流动特性、湍流对等离子体炬内等离子体特性的影响， 以及等离子体炬运行参数对等离子体特性的影响.将数值模拟结果与已有的实验结果进行了 比较. 关键词： 等离子体炬 磁流体力学 数值模拟     

活性聚苯乙烯膜诱导碳酸钙异相成核结晶

0引言生物矿物材料(如骨、牙齿、贝壳等)的优异性能[1]使得无机材料的仿生合成(又称有机模板合成)成为近年来研究的热点之一[2]。该合成技术的优点是,通过有机物分子与无机离子的相互作用,能够在温和的条件下合成出具有多级结构、特殊形貌和优异性能的有机/无机复合材料。CaCO3     

色谱法在三氯半乳蔗糖合成中的应用

采用薄层色谱和柱色谱法，选择优化展开体系，有效地分析了三氯半乳蔗糖中间体2，3，6，3′，4′-五氧乙酰蔗糖混合物，并证实该混合物中杂质为三苯甲醇，为三氯半乳蔗糖的合成研究取得了重要发现。     

Synthesis, Crystal Structure and Antibacterial Activity of Two Hydrazones Derived from 2-Fluorobenzhydrazide

Two new Schiff base benzoyl hydrazone compounds, C14H10FN3O3 (Ⅰ) and C14H10F2N2O (Ⅱ), have been synthesized and characterized by elemental analysis, IR, UV and X-ray single-crystal diffraction. Both compounds crystallize in monoclinic, space group P21/c with a = 7.0514(14), b = 25.928(5), c = 7.7099(15), β = 111.823(2)°, V = 1308.6(4)3, Z = 4, C14H10FN3O3, Mr = 287.25, Dc = 1.458 g/cm3, μ(MoKα) = 0.115 mm-1, F(000) = 592, the final R = 0.0841 and wR = 0.2489 for 1901 observed reflections (I > 2σ(I)) for I; a = 11.232(3), b =12.735(4), c = 8.612(2) , β = 90.869(3)°, V = 1231.7(6)3, Z = 4, C14H10F2N2O, Mr = 260.24, Dc = 1.403 g/cm3, μ(MoKα) = 0.111 mm-1, F(000) = 536, the final R = 0.0453 and wR = 0.1085 for 1317 observed reflections (I > 2σ(I)) for Ⅱ. The antibacterial activities of both compounds against two bacteria were first studied and one compound showed considerable antibacterial activity against K. Pneumonia and S. aureus.     

8×8APD阵列激光三维成像接收机研制

为了实现对目标的无扫描阵列激光三维成像并研究系统参数对三维成像距离分辨率的影响,研制了8×8 pixel激光三维成像接收机。接收机采用线性模式APD阵列,设计了模拟信号放大、阈值处理将回波光信号转换为数字信号后,利用FPGA设计实现64通道高精度阵列计时系统,实现了对目标的无扫描实时三维成像功能。首先对设计完成的三维成像接收机组成及成像原理进行了介绍,对三维成像接收机中APD探测器阵列信号的模拟处理和数字处理流程和实现方式进行了说明。随后分别对三维成像的核心FPGA计时系统及探测器整体进行了电子学测试和实验测试。测试结果表明,FPGA计时子系统的时间分辨率优于140 ps,三维成像系统整体距离分辨率在0.2 m左右。最后对分辨率的误差进行了分析,结果表明,激光回波强度波动是影响此接收机距离分辨率的最主要因素。     

Simultaneous measurement of SO_2 and NO_2 concentration using an optical fiber-based LP-DOAS system

SO2 and NO2 are the most important pollution in atmosphere.An optimized long path(LP)differential optical absorption spectroscopy(DOAS)system of high light intensity at an ultraviolet(UV)wavelength is proposed and used to measure the concentration of SO2 and NO2 simultaneously.In contrast to the traditional DOAS,the system adopted a Y-type optical fiber structure instead of a combination of mirrors in the telescope.The UV light intensity test shows that the light intensity of UV can arrive to above 80% of the max measuring range when the light path reaches 135 m,and the integral time of the spectrograph is only 15 ms.The system is proved to be efficacious through laboratory calibration.The maximum error of SO2 calibration is 4.19%,and is 5.22% for NO2.The error of the SO2 and NO2 mixture calibration is within 10%.Field measurement is implemented in a wastewater treatment plant in winter.The measurement light path is 738 m.The concentration of SO2 varies from 6μg/m^3(2.26 ppb)to 20μg/m^3(7.52 ppb),and the concentration of NO2varies from 100μg/m^3(53.2 ppb)to 200μg/m^3(106.4 ppb)approximately.The results are in accordance with the data from a monitoring station nearby in magnitude order and variation tendency mostly.     

分析用标准样品氟铃脲的合成、纯化及表征

合成了氟铃脲农药粗品,通过活性炭吸附、重结晶进行初步纯化;然后采用柱层析分离技术,以硅胶为填料,乙酸乙酯／石油醚（30～60℃）（1：3,V／V）为展开剂（Rf≈0．5）进行提纯。用紫外光谱（UV）、红外光谱（IR）、核磁共振（^1H NMR,^13C NMR）及质谱（MS）进行了结构表征;以高效液相色谱法测得该试样纯度在99％以上。     

CdS形貌可控制备及其可见光分解水产氢性能

以还原型谷胱甘肽(GSH)作为硫源和结构导向剂水热法“一壶”制备系列硫化镉(CdS)光催化材料,采用透射电镜(HRTEM)、场发射扫描电镜(FESEM)、X射线衍射仪(XRD)、紫外可见漫反射(UV-Vis)、荧光光谱(PL)、比表面分析仪(BET)和光解水产氢反应等对催化材料的微观表面结构、光吸收性能以及光催化性能进行了研究。结果表明：通过调节反应物的nCd/nS比和水热温度等参数可控的制备出分散性好的CdS实心纳米球(s-CdS)、空心纳米球(h-CdS)以及纳米棒(r-CdS)等不同微观形貌的光催化材料。对比研究了不同形貌光催化剂的光解水产氢的宏观性能,发现s-CdS产氢活性最高,h-Cd次之,r-CdS最差。这一结果可归结于构成实心球表面亚微晶的粒径相比其它形貌的小,导致电子-空穴对快速迁移至表面并与溶液反应,抑制体相复合,导致生成的氢气量大大的提高。     

火焰原子吸收法测定化妆品中的铬

采用火焰原子吸收分光光度法测定了兰州市的一些市售化妆品中铬的含量。结果表明,方法检测限(3σ)为0.003 mg/L,回收率在94%~105%之间,相对标准差小于1.3%,方法简便快速;市售多数化妆品中的铬含量超过国家标准,须引起人们的注意。     

Strong Correlation of Fluorescence Photons without Quantum Interference

It has been predicted that a driven three-level V atom can emit strongly correlated fluorescence photons in the presence of quantum interference. Here we examine the effects of quantum interference on the intensity correlation of fluorescence photons emitted from a driven three-level A atom. Unexpectedly, strong correlation occurs without quantum interference. The quantum interference tends to reduce the correlation function to a normal level. The essential difference between these two cases is traced to the different effects of quantum interference on coherent population trapping （OPT）. For the V atom, quantum interference and coherent excitation combine to lead to OPT. For the A atom, however, the quantum interference tends to spoil OPT while the coherent excitation induces the effect.