校正矩阵同时分光光度法测定人发中钙、镁、锌

将校正矩阵计算法应用于分光光度法中,同时测定了人发中的钙镁锌含量。讨论了方法原理和最佳实验条件,对４个发样和模拟样进行了测定,取得满意结果。     

铬(Ⅵ)-三溴偶氮胂-HNO3催化动力学光度法测定痕量铬的研究

研究了铬（Ⅵ）对硝酸氧化三溴偶氮胂（ＴＢＡＡ）褪色反应的催化作用及其动力学分析,建立了测定痕量铬的新方法。检出限可达ｎｇ级,线性范围０－２．５μｇＣｒ（Ⅵ）／５０ｍＬ,表观摩尔吸光系数５．４＊１０＾５Ｌ．ｍｏｌ＾－１．ｃｍ＾－１。方法简便,灵敏、快速、准确,已用于铸铁标样和人发样品中痕量铬的测定,结果满意。     

X-ray observations of tungsten wire array Z-pinch implosions on QiangGuang-1 facility

Z-pinch experiments with two arrays consisting, respectively, of 32 4-μm- and 6-μm-diameter tungsten wires have been carried out on QiangGuang-1 facility with a current rising up to 1.5MA in 80ns. At early time of implosion, x-ray framing images show that the initial emission comes from the central part of arrays, and double clear emission rings, drifting to the anode and the cathode at 5×10⁶cm/s and 2.4×10⁷cm/s respectively, are often produced near the electrodes. Later, in a 4-μm-diameter tungsten wire array, filamentation caused by ohmic heating is prominent, and more than ten filaments have been observed. A radial inward shift of arrays starts at about 30\,ns earlier than the occurrence of the x-ray peak power for both kinds of arrays, and the shrinkage rate of emission region is as high as 1.7×10⁷cm/s in a 4-μm-diameter tungsten wire array, which is two times higher than that in a 6-μm one. Emission from precursor plasmas is observed in implosion of 6-μm-diameter tungsten wire arrays, but not in implosion of a 4-μm-diameter tungsten wire array. Whereas, in a 4-μm-diameter tungsten wire array, the soft x-ray emission shows the growth of m=1 instability in the plasma column, which is caused by current. The reasons for the discrepancy between implosions of 4-μm- and 6-μm-diameter tungsten wire arrays are explained.     

丝阵Z箍缩实验1维X光辐射功率分布

 在Angara-5-1联合实验中,利用条纹像机和光纤阵列实现时间分辨和1维空间分辨,得到了丝阵条纹像,观察到丝阵负载箍缩区X光辐射的1维轴向空间分布信息随时间的演化过程,考察了内爆的同步性和均匀性。通过对比不同结构负载内爆等离子体X光1维时空分布信息,发现由于内层等离子体对磁流体瑞利-泰勒不稳定性的抑制作用,(40+20)根双层钨丝阵比60根单层钨丝阵的内爆轴向同步性好,产生的X光辐射功率高;由于负载存在弯曲、断丝、扭曲等现象,(60+30)根双层钨丝阵比90根单层钨丝阵的轴向同步优势不明显;轴向同步性好与辐射功率高之间存在相关性;辐射波形前沿较快时,X光功率较高。     

快中子照相中的点扩展函数计算

 快中子照相中,基于反冲核原理探测快中子的有机闪烁体平板是普遍采用的快中子辐射转换体。模拟了D-T中子垂直入射BC400闪烁体平板,计算了不同厚度平板闪烁体的点扩展函数,对14.1 MeV快中子照相中闪烁体固有分辨率随厚度的变化进行了研究。计算结果表明,在不考虑二次中子与闪烁体作用及背景噪声等情况时,点扩展函数几乎不依赖于闪烁体厚度。同时,计算还表明在一定的分辨率范围内,由于荧光收集效率的限制,闪烁体厚度增加并不会改善图像对比度。     

激光斑点漂移的研究

用激光照射粗糙表面时,可以观测到颗粒状的细小斑点,当人眼或相机移动时,观测到斑点也发生移动.分析了激光散斑产生和漂移的原因,将散斑漂移简化为几何光学和波动光学问题,得到一致的散斑漂移速度计算公式.利用Mathematica计算光强关联函数,证实圆斑越大散斑越小.实验测量了散斑漂移速度与相机移动速度的关系,结果符合理论公...     

藏药材白花龙胆花中微量元素的分析

对藏药材白花龙胆花中17种微量元素（Cu、Zn、Fe、Mn、Co、Ni、Se、Cr、Mg、Ca、K、Na、P、As、Hg、Pb、Cd）的含量作了测定。结果表明,白花龙胆花中含有较高的人体必需微量元素和常量元素,其中常量元素K、Ca、Na、Mg和微量元素Zn、Fe、Mn的含量均较高。     

康普顿相机图像重建中的快速滤波反投影算法

提出一个由CZT像素探测器与NaI闪烁体阵列组成的康普顿相机，计算探测器系统的几何参数、散射体探测器的能量分辨率及多普勒展宽等因素对相机空间分辨率的影响.相机的总体角分辨率为5.1°~5.6°，主要影响因素为探测器系统的几何参数.首先用解析方法研究图像重建中的滤波反投影算法，不考虑展宽影响时点源重建图像的角分辨率可达1.7°，考虑展宽影响时角分辨率可达4.2°；然后利用Geant4程序进行模拟，用实际应用方法对模拟数据进行重建，不考虑展宽影响时的角分辨率为1.7°，考虑展宽影响时角分辨率可达5.1°.采用滤波反投影算法进行图像重建时，在OpenCL框架下利用GPU实现并行加速，加速比为79倍.     

音乐胎教中的声学问题和人体透声的实验测量

利用声音(音乐)进行胎教有根据吗?即空气中的声音能够透入人体吗?通过模拟实验和人体透声的直接测量,回答是肯定的.实验结果表明,声波从空气中透入人体后,衰减呈低通特性.1000Hz以内 的声波衰减在10dB左右,高于2000Hz的声波衰减大于20dB.为了有效地将声波传入人体,可以采取与人体直接耦合的方法来实现.     

CRYSTAL AND MOLECULAR STRUCTURES OF TWO ISOMERS OF DIETHYL 2, 3-DICYANO-2, 3-DIPHENYLSUCCINATE

Diethyl 2, 3-dicyano-2, 3-diphenylsuccinate was prepared through the oxidative coupling of ethyl α-cyanophenylacetate with Cu~(++)-TMEDA-O_2 system. The product gave, upon chromatography, two crystalline compounds 1 and 2. The single crystals of 1 and 2 were identified by X-ray crystallographic analysis to be meso-and racemie-diethyl 2,3-dicyano-2,3-diphenylsuccinate respectively. It is noteworthy that in the molecules of 1 and 2 there is a remarkable lengthening effect of the bond length for the central C—C bond, i. e. 1: 1.585; 2: 1.62. It is also observed that there is steric hindrance between the substituent groups attached to the two carbon atoms of the central C—C bond respectively. These data provide the structural basis for the facile dissociation into radicals and the action of polymerization initiator of the title compound. CNDO/2 calculation of charge density and Wiberg bond order for compound 1 yields the results, which are consistent with the crystallographic data.