层流与湍流等离子体冲击射流特性比较

本文采用数值模拟方法,对层流与湍流氩等离子体射流在空气环境中冲击平板时的流动与传热特性进行了对比研究.结果表明,在平板和射流进口间的距离较大时,平板的存在只对其附近的射流参数分布有较大影响,层流等离子体冲击射流的温度与轴向速度的轴向梯度明显小于湍流等离子体冲击射流情形;由于在平板表面形成的径向壁面射流对引射的附加贡献,层流和湍流等离子体冲击射流对环境空气的引射量明显增加.     

K+和Al3+掺杂对掺Er3+溶胶凝胶玻璃发光特性的影响

通过Sol-gel(溶胶-凝胶)技术,首次将Al3 离子和K 离子同时引入到掺Er3 硅酸盐玻璃中,并测定了硅基玻璃中Er3 离子的吸收光谱、透射光谱、光致发光光谱(PL谱)、上转换光谱、拉曼光谱及荧光寿命.结果显示:掺入的Al3 离子和K 离子不但分别使Er3 离子的荧光强度增强20倍和70倍,而且使Er3 离子在1 532 nm处的荧光寿命从4.8 ms延长至7.1和11.2 ms,但经过进一步分析可知两者对其的影响机制却完全不同;同时作者发现,在980 nm波长激发下,Er3 离子的上转换荧光应该同时存在两种发光机制:双光子吸收和能量传递上转换.     

喷雾热解法制备的SrWO4膜的阴极射线发光

利用超声喷雾热解法制备了钨酸锶SrWO₄多晶发光膜,并研究了制备条件及掺杂对其阴极射线发光特性的影响.生成的发光膜在300℃以上退火后具有白钨矿结构,其阴极射线发光为一宽带的蓝光,包括一个位于448nm的蓝色发光带和一个位于488.6nm的蓝绿色发光带,是由阴离子络合物WO₄^2-的电荷转移跃迁引起的.发光强度随着退火温度的升高而增强,而退火气氛对其影响不大.在SrWO₄膜中掺入银离子Ag⁺和镧离子La³⁺后,不影响其发光特性,但铕离子Eu³⁺的掺入对发光特性有影响.     

发光二极管放电实验现象分析

利用直流电源对发光二极管(LED)的结电容充电,切断直流电源后对LED的电压-时间特性进行测量。当充电电压低于LED复合发光的门槛电压,LED的电压-时间特性与普通二极管的相似。当充电电压高于LED复合发光的门槛电压,首次观察到:开始放电的瞬间会出现一个快速下降过程,快速下降到门槛电压以下;LED上的电压越高,快速下降到的电压越低。对该现象进行分析,得到一些新的结论。当LED的正偏电压高于复合发光的门槛电压后,出现了注入到扩散区的非平衡载流子随正偏电压的提高而减小的现象,即dQ/du<0。     

梯度表面能材料上液滴运动特性实验

对水平和30°倾角放置梯度表面能材料表面上液滴运动特性进行了可视化实验,分析了液滴在梯度表面上运动速度的变化规律,以及液滴大小和表面倾角对运动速度变化的影响.实验结果表明:在梯度表面能材料上,液滴能获得较大的宏观运动速度,并可以沿30°倾角放置的梯度表面材料上自下而上的运动;大液滴较小液滴的峰值运动速度大,运动距离更远;液滴在运动过程中出现蠕动的现象.     

MCeO3：Eu^3＋（M=Sr，Ba）的合成及发光性质研究

利用高温固相反应法合成了Eu^3＋掺杂的MCeO3（M=Sr，Ba）发光粉末样品，采用X射线衍射技术和荧光光谱等测试手段分别对其物相组成和发光性质进行了研究。X射线衍射结果显示，Eu^3＋离子容易替代MCeO3晶格中M^2＋离子的位置。荧光光谱测试结果表明，Eu^3＋掺杂的SrCeO3和BaCeO3样品在紫外波段存在着非常宽的吸收带，峰值分别位于311和320nm左右，它们属于Ce^4＋-O^2-的电荷迁移带，SrCeO3和BaCeO3基质与Eu^3＋离子之间存在着能量转移。在MCeO3：Eu^3＋样品中，Eu^3＋的发射主要来自于^5D0激发态能级，其中以磁偶极跃迁^5D0-^7F1发射强度为最大；此外样品中还存在着较高的^5D1激发态能级的辐射跃迁。SrCe03：EU^3＋样品的发射强度远大于BaCeO3：EU^3＋样品。     

CdS/TiO2/漂珠复合光催化剂制备及其降解高效氯氰菊酯研究

采用溶胶-凝胶-浸渍法制备了Cds/TiO2/漂珠复合光催化剂,通过SEM,XRD对其结构进行了表征.以高效氯氰菊酯(BEC)杀虫剂的光催化降解为模型反应,研究了CdS/TiO2/漂珠的光催化性能,探讨了影响催化剂活性的因素及采用太阳光作光源处理BEC的可行性.结果表明,CdS/TiO2/漂珠投加量为3 000mg·L-1,初始浓度为45 mg·L-1、初始pH为6.5,通气量为200 mL·min-1时间为60 min,BEC降解率分别为92.1%(125W高压汞灯)和79.3%(5 W紫外灯),采用太阳光照射300 min,BEC降解率可达93.4%.BEC的降解反应遵从L-H动力学模型,测得反应速率常数9.80 mg·(L·min)-1,吸附常数4.36×10-3 L·mg-1.     

Resonant Response of Rectangular/kFM Cantilever in Liquid

Dynamic characteristics of atomic force microscopy （AFM） cantilevers can be influenced by their working media. We perform an experimental study on the resonant responses of rectangular AFM cantilevers with different sizes immersed in various viscous fluids. The measured resonance frequencies in liquids are used to valldate several theoretical models. Comparison shows the analytical model proposed by Sader [J. Appl. Phys. 84 （1998） 64] can give the best agreement with the experimental results with the maximum relative error nearly 16% for all the cantilevers in different liquids. The ratio between the resonant frequencies in air and water is almost independent of the cantilever length, which is consistent with the theoretical analyses.     

Monte Carlo Simulation of Optical Properties of Wake Bubbles

Based on Mie scattering theory and the theory of multiple light scattering, the light scattering properties of air bubbles in a wake are analysed by Monte Carlo simulation. The results show that backscattering is enhanced obviously due to the existence of bubbles, especially with the increase of bubble density, and that it is feasible to use the Monte Carlo method to study the properties of light scattering by air bubbles.     

Dynamics of Efficiency Change by Temperature in Diode Pumped Nd：YAG Heat Capacity Laser

We investigate the influence of temperature on the efficiency of diode pumped Nd：YAG heat capacity laser is studied. It is shown that the efficiency of such a laser system is greatly reduced at higher temperature. This bad behaviour is mainly caused by the doped-ion redistribution among various Stark levels of the ground state, and by a thermal equilibrium between the upper laser level and the pump level. Meanwhile, the thermal excitations from the ground state to the lower laser level also play a role. We derive a model to describe those effects, with the considerations of emission spectrum of laser diodes, the subtle Stark structures and the linewidth of absorption and of simulated-emission.