表面修饰的二氧化锡纳米粒子的制备及微结构表征

采用胶体化学制得表面包覆有ＤＢＳ的二氧化锡纳米粒子，并运用一系列手段对其微结构进行了表征。     

Effect of Variant Counterions on Stability and Particle Size of Silica Sol

The effects of variant counterions with ionic strength of 0.05, 0.10, 0.20 and 0.25 mol·kg^-1 on the stability and particle size of silica sols have been studied using the traditional methods of Ubbelohde viscosity measurement, TEM and titration respectively, finding that the stability and particle size of the silica sols are all concerned with the acidic, positively electric properties and the sizes of the counterions, as well as the attraction between the counterions and surface silicon hydroxyl groups of the silica sols. The small positively charged counterions lead to the decrease in particle sizes, making the silica sol the most stable. But the larger weakly acidic counterions can restrict the particle sizes of the silica sols and easily make the sols coagulate. It was also found that there existed a linear relationship between log r and log η, which has not ever been reported. The effect of temperature on the stability and particle sizes was also discussed.     

TiO2-双亲共聚物复合纳米粒子的合成与紫外光敏特性

用偶联剂乙烯基三乙氧基硅烷改性纳米粒子TiO₂, 应用超声技术将TiO₂ 纳米粒子分散在甲醇介质中, 然后用苯乙烯(ST)原位聚合包封, 再用丙烯酰胺或乙烯基吡咯烷酮(VP)共聚, 两步原位分散聚合得到了有机聚合物为壳、TiO₂为核的有机/无机复合粒子. 用红外光谱、紫外-可见光谱、透射电子显微镜等检测手段进行表征. 结果显示: 由于双亲共聚物对TiO₂纳米粒子的敏化作用, 紫外-可见光谱图上两种纳米复合粒子的最大吸收峰均有明显红移, 并且吸收光谱的范围扩大了, 其中尤以TiO₂/(PST-co-PVP)为甚. 意味着光敏化活性的提高, 特别是在可见光谱的范围内. 这种情形对宽带隙半导体材料如TiO₂纳米粒子的光催化特性是有利的, 表明这类材料的应用空间得到了拓展.     

硒化镉纳米粒子与碘化三甲氨基苯基卟啉钻复合膜光学性能研究

为了探索CdSe纳米粒子合成的最佳条件及其与碘化三甲氨基苯基卟啉钴（CoTAPPI）复合膜的光学性能，采用湿化学法合成了CdSe纳米粒子；利用逐层沉积法组装了CdSe—CoTAPPI复合膜。用紫外-可见吸收光谱监测了成膜过程。利用荧光光谱比较系统地研究了聚苯乙烯磺酸钠（PSS）、放置时间、热处理、紫外光照射等条件对复合膜发光性能的影响，结果发现复合膜的发光性能相对于单一组份的CASe纳米粒子和CoTAPPI都有很大程度改变。     

我国物质结构研究的大型实验平台(续)——非加速器粒子物理实验设施

在粒子加速器问世以前,科学家就利用天然放射性和宇宙红进行核物理的研究。1919年卢瑟福用放射性物质产生的α射红轰击原子核,首次实现了人工核反应。天然放射性粒子来之不难,但能量较低、强度很弱;宇宙红能量最高可达1022eV,却是"靠天吃饭",难以开展精确的实验。粒子加速器在20世纪30年代初发明后,很快成为核物理和粒子物理研究的主角。然而,随着粒子物理向高能量前沿的推进,加速器的规模成越来越大,位于瑞士和法国边境质心系1     

圆锥曲线焦点弦的一个性质的推广及简洁证明

文[1]介绍了圆锥曲线焦点弦的一个性质,本文对这个性质进行推广得到3个命题.命题1如图1,     

水中镉化合物粒子消光系数及其反射率光谱(400～900nm)测量

测量出水中镉化合物单位浓度消光系数光谱曲线和镉化合物干燥环境下的反射率光谱曲线是水体镉元素含量遥感反演的关键。首先采用自主设计的透射光测量装置,利用Analytical Spectral Devices(ASD)光谱仪分别测量了相同厚度不同浓度的两种镉化合物粒子溶液(硫化镉和氧化镉)的透射光辐亮度,通过比值法计算出不同浓度的镉化合物粒子溶液的消光系数,最终得到其400~900nm波长范围内的单位浓度消光系数光谱。然后再利用ASD光谱仪在户外晴好干燥的环境下对这两种镉化合物的反射率光谱进行了测量,为日后进一步计算其单位浓度吸收和散射系数打下基础。单位浓度消光系数光谱测量结果表明,硫化镉在675nm出现极大值,在550和830nm出现极小值;氧化镉则随着波长的增加呈逐渐减少的单调趋势;两种化合物在水中的消光作用主要在紫蓝光波段。反射率光谱测量结果表明,硫化镉的反射率从500nm开始快速增大至650nm后趋于平缓;氧化镉从525nm开始呈近线性递增至900nm;二者都具有明显的光谱特征。本文在国内首次专门针对水质遥感领域开展了具有光活性的镉化合物的光学参数测量工作,并获得了这两种化合物的单位浓度消光系数和反射率光谱曲线,是水体镉含量遥感反演模型所必需的光学参数之一,为镉含量遥感反演这一难题提供一个突破口,测量结果可以为镉含量提取的遥感工作波段选择提供有力的参考依据,同时也为水体镉含量的遥感提取提供了模型必需的重要参数。     

用particular制作下雨场景

在许多的电影电视片头或者片中特效中,经常会用到particular插件生成的粒子来制作的逼真特效。本文就用particular插件来模拟下雨场景,并在场景中增加真实的背景,使下雨更加真实。     

Application of DEM modified with enlarged particle model to simulation of bead motion in a bead mill

We applied the discrete element method （DEM） of simulation modified by an enlarged particle model to simulate bead motion in a large bead mill. The stainless-steel bead mill has inner diameter of 102 mm and mill length of 198 mm. The bead diameter and filling ratio were fixed respectively at 0.5 mm and 85%. The agitator rotational speed was changed from 1863 to 3261 rpm. The bead motion was monitored experimentally using a high-speed video camera through a transparent mill body. For the simulation, enlarged particle sizes were set as 3-6 mm in diameter. With the DEM modified by the enlarged particle model, the motion of enlarged particles in a mill was simulated.The velocity data of the simulated enlarged particles were compared with those obtained in the experiment. The simulated velocity of the enlarged particles depends on the virtual frictional coefficient in the DEM model. The optimized value of the virtual frictional coefficient can be determined by considering the accumulated mean value. Results show that the velocity of the enlarged particles simulated increases with an increase in the optimum virtual frictional coefficient, but the simulated velocity agrees well with that determined experimentally by optimizing the virtual frictional coefficient in the simulation. The computing time in the simulation decreases with increased particle size.