南海红树林内生真菌ZSUH 36次级代谢物的分离鉴定

红树林;内生真菌;次级代谢产物;抗肿瘤活性     

低剪切混合方法制备炭黑/聚丙烯纳米复合材料及其电性能研究

采用一种在低剪切应力场下纳米复合材料的加工方法,制备得到纳米炭黑(CB)粒子在聚丙烯(PP)中以纳米尺度分散的聚合物导电复合材料.扫描电镜观察表明CB粒子在纳米复合材料中以纳米尺度存在,并均匀的分布在PP基体中.电性能测试发现,通过这种低剪切混合方法得到的纳米复合材料具有非常低的导电逾渗阈值(vc=2.49vol%)和较高的临界电阻指数(t=5.82),很大的偏离了普适逾渗理论.基于隧道逾渗模型对体系的电导率进行了模拟,并对CB的分散状态与导电网络的关系进行了分析.发现当纳米CB粒子以纳米尺度分散于基体中时,并不遵从接触导电机理,而是隧道逾渗机理在CB/PP纳米复合材料中起主导作用.     

铜离子在CuLaHY分子筛中的分布与吸附脱硫性能

在空气气氛中采用等体积浸渍法制备了具有不同Cu担载量的CuLaHY分子筛吸附剂, 并用X射线衍射(XRD)、比表面积(BET)、X射线光电子能谱(XPS)技术对分子筛吸附剂进行了表征. 通过多晶XRD确定了Cu2+及La3+离子在Y型分子筛笼内的结构与分布, 并测定了分子筛吸附剂在含二苯并噻吩(DBT)的模拟柴油中的吸附脱硫性能. 结果表明, 前驱体CuCl2中的大部分Cu物种与LaHY分子筛进行了离子交换, 进入分子筛笼内, 极少部分Cu物种以CuCl形式高度分散在Y型分子筛的笼中. La3+离子及进入Y型分子筛笼中的部分Cu2+离子处于茁笼的SI'位, 而另一部分Cu2+离子与骨架氧和水分子配位, 并牢固地定位于Y型分子筛超笼中的SII及SIII位上. 处于超笼中SII及SIII位上的Cu2+离子对模拟柴油中的DBT分子具有吸附作用, 成为吸附脱硫的中心. 当模拟柴油中有萘存在时, 与DBT分子会产生竞争吸附.     

水溶性羟基丙烯酸酯树脂的合成

以氧化苯甲酰为引发剂,通过溶液聚合合成了水溶性丙烯酸丁酯-甲基丙烯酸甲酯-丙烯酸-甲基丙烯酸羟乙酯四元共聚物,其结构经~1H NMR,~(13)C NMR和IR表征,热分析结果表明其分解温度为360 ℃～440 ℃.     

梳型聚合物在固液界面吸附形态的Monte Carlo模拟

采用Monte Carlo模拟方法对PAA/PEO梳型聚合物在固液界面吸附形态进行了模拟,得到了聚合物在液相中聚集形态以及在固液界面上吸附形态的瞬时构型,同时获得了聚合物的吸附层厚度、均方回转半径和吸附在固液界面的各种链段数等微观信息. 结果证实：随着聚合物的接枝数Np增大,聚合物在液相中的扩散系数逐渐降低、相对粘度逐渐增大;当Np≥6时,羧基阴离子基团置于吸附层最外围,吸附层厚度近似等于PEO侧链长度,聚合物在固体表面形成空间排斥为主、静电排斥为辅的吸附状态;吸附聚合物分子密度过低或过高均不能起到良好的空间屏蔽或阻隔效应;吸附在固体粒子表面聚合物应该具有适宜的吸附-脱附自平衡能力.     

微通道背板热管系统最佳充液率实验研究

为研究不同工况和工质对微通道背板热管系统最佳充液率的影响,设计系统充液率实验,通过分析充液率对换热量、背板竖向出风温度分布、蒸发器及冷凝器进出口工质温度及压力的影响,确定不同条件下的系统最佳充液率。结果表明:1)标准工况下,采用R22工质的系统最佳充液率为65%~75%,背板竖向各位置出风温度最低,蒸发器进出口工质温差达到最小;2)系统最佳充液率随着背板进风温度的上升而增大,进风温度超过40℃后,最佳充液率保持不变;3)系统最佳充液率随冷凝器进水温度的降低而增大;4)R134a系统和R22系统最佳充液率基本一致,最大换热量不同。     

分子印迹电化学传感器的制备及其快速检测饮水中草甘膦残留的应用研究

以吡咯(Py)为功能单体,草甘膦(Gly)为模板,采用电化学聚合法构建了草甘膦分子印迹电化学传感器。通过循环伏安法(CV)、差分脉冲伏安法(DPV)、电化学交流阻抗法(EIS)对印迹电极性能进行了表征,筛选了印迹电极的聚合体系和模板分子的洗脱方法,优化了检测体系的p H值和吸附时间等。结果表明,以铁氰化钾为电活性探针,在最优检测体系中该印迹传感器对草甘膦具有特异性快速响应、灵敏度高和稳定性好的优点,传感器的峰电流与草甘膦浓度在5~800 ng/m L范围内呈良好的线性关系,相关系数(r2)为0.981 7,检出限(S/N=3)为0.27 ng/m L。该传感器具有良好的重现性和稳定性,放置3周后对目标物的响应峰电流无明显变化。用于实际样品中草甘膦的测定,加标回收率为78.6%~99.0%,能满足现场快速检测的要求。     

Spectroscopic properties of Yb~(3+)-doped TeO_2–BaO–BaF_2–Nb_2O_5-based oxyfluoride tellurite glasses

A series of oxyfluoride glasses with the compositions of 75 mol% TeO2, 10 mol% Nb2O5,(15 mol%-x) BaO, x BaF2(x = 0 mol%, 5 mol%, 10 mol%, 15 mol%) doped with Yb2O3 were prepared by the melt-quenching method. Their emission cross-sections, fluorescence lifetimes, and gain properties were investigated by using the absorption spectra and the fluorescence decay curves. The results show that by substituting BaF2 for BaO, the emission cross-section decreases from 1.37 pm2 to 1.21 pm2, and the fluorescence lifetime increases from 0.71 ms to 0.96 ms. These properties indicate that this oxyfluoride tellurite glass may have potential uses as the Yb2O3-doped gain medium in a solid laser.     

Improved design and construction of an ionization chamber for the CSNS beam loss monitor (BLM)

Based on the first ionization chamber (IC) prototype, the structure, working gas component and electrode material of the IC are improved. The test of the improved IC shows that the plateau length is about 2000 V, the plateau slope is less than 0.2%/100 V, the sensitivity is 19.6 pA/rad·h^-1, the up-limitation of the linearity can be up to 3.6×10⁵ rad/h, and the applied voltage can be operated to 3500 V. The test results show that the performance of the improved IC meets the requirements of the beam loss monitor.     

Interference effects on the photoionization cross sections between two neighbouring atoms: nitrogen as an example

Interference effects on the photoionization cross sections between two neighbouring atoms are considered based on the coherent scattering of the ionized electrons by the two nuclei when their separation is less than or comparable to the de Broglie wave length of the ionized electrons. As an example, the single atomic nitrogen ionization cross section and the total cross sections of two nitrogen atoms with coherently added photoionization amplitudes are calculated from the threshold to about 60~\AA (1~\AA=0.1~nm) of the photon energy. The photoionization cross sections of atomic nitrogen are obtained by using the close-coupling R-matrix method. In the calculation 19 states are included. The ionization energy of the atomic nitrogen and the photoionization cross sections agree well with the experimental results. Based on the R-matrix results of atomic nitrogen, the interference effects between two neighbouring nitrogen atoms are obtained. It is shown that the interference effects are considerable when electrons are ionized just above the threshold, even for the separations between the two atoms are larger than two times of the bond length of N₂ molecules. Therefore, in hot and dense samples, effects caused by the coherent interference between the neighbours are expected to be observable for the total photoionization cross sections.