Brazing 6061 aluminum alloy with Al-Si-Zn filler metals containing Sr

Al-6.5Si-42Zn and Al-6.5Si-42Zn-0.09Sr filler metals were used for brazing 6061 aluminum alloy. Air cooling and water cooling were applied after brazing. Si phase morphologies in the brazing alloy and the brazed joints were investigated. It was found that zinc in the Al-Si filler metals could reduce the formation of eutectic Al-Si phase and lower the brazing temperature at about 520℃. Adding 0.09wt% Sr element into the Al-6.5Si-42Zn alloy caused α-Al phase refinement and transformed acicular Si phase into the finely fiber-like. After water cooling, Zn element dissolved into the Al-Si eutectic area, and η-Zn phase disappeared in the brazed joints. Tensile strength testing results showed that the Sr-modified filler metal could enhance the strength of the brazed joints by 13% than Al-12Si, while water-cooling further improved the strength at 144 MPa.     

Thermoelectric effect of silicon films prepared by aluminum-induced crystallization

Aluminum-induced crystallized silicon films were prepared on glass substrates by magnetron sputtering. Aluminum was added in the silicon films intermittently by the regular pulse sputtering of an aluminum target. The amount of aluminum in the silicon films can be controlled by regulating the aluminum sputtering power and the sputtering time of the undoped silicon layer; thus, the Seebeck coefficient and electrical resistivity of the polycrystalline silicon films can be adjusted. It is found that, when the sputtering power ratio of aluminum to silicon is 16%, both the Seebeck coefficient and the electrical resistivity decrease with the increasing amount of aluminum as expected; the Seebeck coefficient and the electrical resistivity at room temperature are 0.185-0.285 mV/K and 0.30-2.4 Ω·cm, respectively. By reducing the sputtering power ratio to 7%, however, the Seebeck coefficient does not change much, though the electrical resistivity still decreases with the amount of aluminum increasing; the Seebeck coefficient and electrical resistivity at room temperature are 0.219-0.263 mV/K and 0.26-0.80 Ω·cm, respectively.     

Tuning the magnetic anisotropy in LSMO manganite films through non-magnetic nanoparticles

We report the observation of anomalous magnetic anisotropy driven by nonmagnetic ZrO2 nanoparticles in epitaxial La2/3Sr1/3MnO (LSMO) films grown on LaAlO3 (LAO) substrates. The compressive epitaxial strain imposed by the lattice mismatch of substrate and film is tuned by the density of ZrO2 nanoparticles embedded in the film matrix and affects the magnetic anisotropy as well as the magnetotransport properties. Epitaxial 54 nm thick LSMO thin films with different concentrations of ZrO2 nanoparticles demonstrate anisotropic hysteresis loops concomitant with anisotropic magnetotresistance behavior. The biaxial epitaxial strain, induced by the substrate/film lattice parameter mismatch is partially relaxed by increasing the density of precipitates and they serve as a tuning parameter for the strain state. We interpret our results by a strain-induced interplay of impurity scattering, weak localization and magnetic domain structure.     

非离子表面活性剂修饰对磁流变弹性体磁流变效应的影响

使用表面活性剂修饰铁颗粒,并测试修饰作用对以天然橡胶为基体的磁流变弹性体磁流变效应的影响．通过磁耦合动态测试仪对材料的剪切性能包括剪切储能模量和损耗因子进行测试,结果表明当材料被Span 80修饰时,剪切储能模量增加量为零场剪切模量的188％,而损耗因子的变化可以忽略．使用扫描电镜观测样品的微结构,结果表明表面活性剂能促进铁颗粒和橡胶基体的融合性,并使铁颗粒形成自组装结构,这种结构有利于相对磁流变效应的提高．     

Magnetic rotation imaging method to measure the geomagnetic field

A new imaging method for measuring the geomagnetic field based on the magnetic rotation effect is put forward. With the help of polarization property of the sunlight reflected from the ground and the magnetic rotation of the atmosphere, the geomagnetic field can be measured by an optical system installed on a satellite. According to its principle, the three-dimensional image of the geomagnetic field can be obtained. The measuring speed of this method is very high, and there is no blind spot and distortion. In this paper, the principle of this method is presented, and some key problems are discussed.     

具有非单调发生率SEIS流行病模型的全局稳定性分析

研究了具有非单调发生率的流行病模型,非单调发生率刻画了某种传染病随着感染人数的增多人们的心理反映对疾病传播的影响.通过对无病平衡点和地方病平衡点的全局稳定性分析,给出了随着时间的推移,疾病灭绝或持续存在的阈值条件.     

虚拟战场特殊效果仿真研究

爆炸、火焰等特殊效果是虚拟战场的重要组成部分,对于提高虚拟战场仿真的逼真度具有重要作用;分析了特殊效果仿真的基本方法,对虚拟战场中的各种特殊效果进行了分类;指出了虚拟战场特殊效果仿真的难点,并给出了具体的解决方法.     

基于热-流体耦合理论对还原炉冷却模块温度场的研究

基于热-流体耦合理论, 采用流体分析软件STAR-CD对还原炉冷却模块进行了流场与温度场耦合数值分析,讨论了水垢厚度、水流速度、水管直径、水温及水管间距对温度场的影响.该模型不仅可以用于冷却模块的设计和耐火材料的选取,还可以用于分析判断冷却模块的损坏程度.     

介质的增益和损耗作用对2MQES光场Y压缩的影响

构造了在增益介质和吸收损耗介质中沿Z方向传播强度相等的2MQES(Two state-superposition multimode quantum entanglement state,2MQES)光场.利用多模压缩态理论,对2MQES光场的广义非线性等幂次N次方Y压缩特性进行了研究,并对介质增益和吸收损耗作用对2MQES光场的广义非线性等幂次N次方Y压缩效应的影响进行了详细探讨.结果表明,介质为增益介质时,增益系数αj＞0, 2MQES光场的广义电场分量和广义磁场分量呈现出N次方Y压缩效应.αj增大,压缩幅度和压缩强度减小;介质为吸收介质时,增益系数αj＜0,此时,2MQES光场的广义电场分量和广义磁场分量也呈现出N次方Y压缩效应,但|αj|增大,压缩幅度和压缩强度也随之增大,且吸收越强,压缩幅度和压缩强度越大.这表明吸收介质对压缩更为有利.     

Thomson离子谱仪参数和实验数据处理

Thomso离子谱仪利用磁场和电场对带电粒子有偏转作用,通过测量偏转的曲率来获得离子种类和离子能量。在激光等离子体相互作用中有多种带电离子,为了得出质子的能谱,常采样Thomson离子谱仪和CR39相结合测量得出质子能谱。在给定谱仪参数下,带入有效磁场,用Thomson抛物线方程作出质子抛物线曲线,与实验中形成的抛物线进行比对,进而确认质子,用matlab编程计算质子能量。