高效液相色谱的4种商品手性柱对38种手性化合物的拆分研究

采用纤维素-三(3,5-二甲基苯基氨基甲酸酯)涂敷型手性固定相(Chiralcel OD柱)、直链淀粉-三(3,5-二甲基苯基氨基甲酸酯)涂敷型手性固定相(Chiralpak AD柱)、直链淀粉-三(3,5-二甲基苯基氨基甲酸酯)键合型手性固定相(Chiralpak IA柱)和Pirkle型的(S,S)-Whelk-01手性固定相对38种外消旋体化合物进行手性拆分。实验结果表明,4种固定相的手性识别能力为:OD>AD>IA>(S,S)-Whelk-01,OD固定相的手性识别率达到60%,并且它们之间的手性识别性能还具有一定的互补性。本研究对4种常用手性固定相的拆分能力进行了对比,为拆分手性化合物时有的放矢地选择手性固定相提供了参考。     

基于MDA法计算水雾粒子红外隐身粒径

水雾隐身技术是一种较为理想且经济适用的目标特征信号控制技术。本文从辐射传输方程出发,考虑水雾粒子的本身辐射和散射,提出以红外表观透射率评价水雾粒子的红外隐身性能。应用Modified Differential Approximation(MDA)法结合MIE理论,计算了水雾粒子红外表观透射率随水雾粒子浓度和粒径的变化关系,得到水雾粒子最佳红外隐身粒径。结果表明:水雾粒子的红外表观透射率随粒子浓度的增加而减小,但当粒子的浓度增加到一定值时,红外表观透射率基本保持不变;水雾粒子的红外表观透射率随粒径的增加先减小后增大,当探测波段为3～5μm时,水雾粒子的最佳红外隐身粒径为6μm;而探测波段为8～12μm时,水雾粒子的最佳红外隐身粒径为12μm。     

A study of the active thermal control for the high energy detector on the HXMT

A thermal control system (TCS) based on the resistance heating method is designed for the High Energy Detector (HED) on the Hard X-ray Modulation Telescope (HXMT). The ground-based experiments of the active thermal control for the HED with the TCS are performed in the ambient temperature range from -15 to 20 ℃ by utilizing the pulse width to monitor the interior temperature of a NaI(Tl) crystal. Experimental results show that the NaI(Tl) crystal's interior temperature is from 17.4 to 21.7 ℃ when the temperature of the PMT shell is controlled within (20±3) ℃ with the TCS in the interesting temperature range, and the energy resolution of the HED is maintained at 16.2% @ 122 keV, only a little worse than that of 16.0% obtained at 20 ℃. The average power consumption of the TCS for the HED with a low-emissivity shell is about 4.3 W, which is consistent with the simulation.     

Syntheses and Crystal Structures of Two Octamolybdate Compounds Modified by CuⅡ-Imidazole Cations

Two new polyoxomolybdate compounds,namely(CuIIL2)2[CuⅡ(HL)2]2[Mo8O26(HL)2].(H2O)4(1) and [CuⅡ(HL)2]2[β-Mo8O26](HL)2(2)(HL=imidazole),were designed and synthesized under hydrothermal conditions.X-ray diffraction analyses reveal that compound 1 consists of one Mo8O26(HL)24-cluster,two CuL2,two Cu(HL)22+,and four disassociated water molecules;and compound 2 is constructed by one β-Mo8O264-cluster,two Cu(HL)22+,and two uncoordinated imidazole molecules.     

钫原子磁偶极超精细结构常数及其同位素的磁偶极矩的理论计算

应用基于B样条基组的相对论耦合簇理论方法,计算了~(212)Fr原子的n S (n=7—12), n P (n=7—12)和n D (n=6—11)态的磁偶极超精细结构常数.与精确实验值的比较说明这套理论方法能精确计算出磁偶极超精细结构常数,其中7P态的磁偶极超精细常数的理论值与实验值之间的差异小于1%.在忽略场移效应对Fr原子7P态超精细结构常数的影响下,通过结合实验值进一步定出了~(207-213,220-228)Fr核磁偶极矩μ,这些值与已有的测量值具有非常好的一致性.本文报道了12S, n P (n=9—12)和n D (n=10—11)态的磁偶极超精细结构常数.     

Electronic States of a Shallow Hydrogenic Donor Impurity in Different Shaped Semiconductor Quantum Wells

The shallow hydrogenic donor impurity states in square, V-shaped, and parabolic quantum wells are studied in the framework of effective-mass envelope-function theory using the plane wave basis. The first four impurity energy levels and binding energy of the ground state are more easily calculated than with the variation method. The calculation results indicate that impurity energy levels decrease withthe increase of the well width and decrease quickly when the well width is small.The binding energy of the ground state increases until it reaches a maximum value,and then decreases as the well width increases. The results are meaningful andcan be widely applied in the design of various optoelectronic devices.     

极化电压对聚丙烯压电驻极体膜压电性能的影响

压电驻极体是具有压电效应的微孔结构空间电荷驻极体材料,其压电性能与材料的微结构和空间电荷密切相关.本文首先利用压缩气体膨化工艺对聚丙烯(PP)的微结构进行改性,然后利用接触极化方法,研究了极化电压与PP膜空间电荷密度之间的关系,及其对压电性能的影响.结果表明对于极化前厚度为100μm的PP膜,其内部建立有序空间电荷分布的阈值极化电压为2 kV;一旦有序空间电荷建立起来,PP膜即具有压电效应.随着极化电压的提高,PP膜的空间电荷密度逐步增大,压电效应显著增强.当峰值电压为8 kV时,PP膜电极上的电荷密度、准静态压电系数和品质因数FOMv(d33·g33)分别为0.56 mC/m2,379 pC/N和8.6(GPa)-1.PP压电驻极体膜的FOMv比聚偏氟乙烯(PVDF)铁电聚合物膜高2个量级以上,且声阻抗非常低(～0.025 MRayl),因此该压电膜在超声波发射-接收系统或脉冲-回波系统中具有明显的优势.     

基于氢键作用由低分子量凝胶因子形成的超分子水凝胶

利用对羟基吡啶及均苯四甲酸合成的超分子单体, 基于分子间氢键作用, 在水中成功地制备出了具有温度响应性的超分子凝胶, 研究了制备条件对凝胶结构的影响.     

Uniaxial experimental study of the acoustic emission and deformation behavior of composite rock based on 3D digital image correlation (DIC)

In this paper, uniaxial compression tests were carried out on a series of composite rock specimens with different dip angles, which were made from two types of rock-like material with different strength. The acoustic emission technique was used to monitor the acoustic signal characteristics of composite rock specimens during the entire loading process. At the same time, an optical non-contact 3 D digital image correlation technique was used to study the evolution of axial strain field and the maximal strain field before and after the peak strength at different stress levels during the loading process. The effect of bedding plane inclination on the deformation and strength during uniaxial loading was analyzed. The methods of solving the elastic constants of hard and weak rock were described. The damage evolution process, deformation and failure mechanism, and failure mode during uniaxial loading were fully determined. The experimental results show that the θ = 0?–45?specimens had obvious plastic deformation during loading, and the brittleness of the θ = 60?–90?specimens gradually increased during the loading process. When the anisotropic angle θincreased from 0?to 90?, the peak strength, peak strain,and apparent elastic modulus all decreased initially and then increased. The failure mode of the composite rock specimen during uniaxial loading can be divided into three categories:tensile fracture across the discontinuities(θ = 0?–30?), slid-ing failure along the discontinuities(θ = 45?–75?), and tensile-split along the discontinuities(θ = 90?). The axial strain of the weak and hard rock layers in the composite rock specimen during the loading process was significantly different from that of the θ = 0?–45?specimens and was almost the same as that of the θ = 60?–90?specimens. As for the strain localization highlighted in the maximum principal strain field, the θ = 0?–30?specimens appeared in the rock matrix approximately parallel to the loading direction,while in the θ = 45?–90?specimens it appeared at the hard and weak rock layer interface.     

Thermally responsive graft copolymer of soy protein isolate and N-isopropylacrylamide: synthesis and self-assembly behavior in aqueous solution

In recent years, soy protein isolate (SPI) has attracted great attention due to its biodegradability, biocompatibility, and wide availability. It has been used in food and pharmaceutical industry such as edible films and drug delivery systems. In this study, we report the synthesis and self-assembly behavior in aqueous solution of thermally responsive graft copolymer (SPI-g-poly(N-isopropylacrylamide) (PNIPA)) of soy protein isolate and N-isopropylacrylamide in aqueous solution. SPI-g-PNIPA was synthesized in the 8 mol/l urea cushioning solution, by using ammonium persulfate as the initiator and mercaptoacetic acid as the protein unfolding agent. Laser light scattering, transmission electron microscopy, and fluorescence spectroscopy have been used to study the self-assembly behavior of SPI-g-PNIPA in aqueous solution. Above the critical micelle concentration (cmc), SPI-g-PNIPA aggregates could assemble into different structures including the simple spherical structure, spherical core–shell structure, and random coil structure, depending on the graft copolymer concentration. The graft copolymer concentration, temperature, pH value, and ionic strength were found to influence the aggregate size and morphology of SPI-g-PNIPA in aqueous solution. With increasing ionic strength, the aggregate size increases. However, pH value, SPI-g-PNIPA concentration, and temperature have complicated influences on the aggregate size. The lower critical solution temperature of the SPI-g-PNIPA at pH 8.5 is 36 °C. The method of intrinsic fluorescence spectroscopy was used for the first time to determine the cmc value of SPI-g-PNIPA in aqueous solution.