ICP-AES测定钛合金中铝、钼和锆的不确定度评定

对钛合金中铝、钼和锆含量测定过程中的不确定度来源进行了辨别,并在此基础上评定了分析结果的不确定度.测量不确定度主要来源于试样称量、标准溶液配制、校准曲线拟合、各种玻璃量器的使用及测量重复性.依据不确定度评定的步骤,计算得到了各分量标准不确定度及合成标准不确定度.     

ICP-OES测定铝质脱氧剂中的铝

试样经高温熔融后,盐酸浸取,采用电感耦合等离子体-发射光谱测定了铝质脱氧剂中的高含量铝.通过试验确定了仪器参数、基体干扰消除等条件.实验结果表明采用基体匹配可消除干扰,保证了样品中高含量铝检测结果的准确度和精密度.该方法快速、准确、稳定性好,其测定结果与化学滴定分析方法的测定值一致.其分析结果能满足生产和科研的需要.     

石墨炉原子吸收光谱法钼涂层直接进样测定葡萄酒中的铝

主要应用了石墨炉原子吸收光谱法塞曼扣除背景方式,在镀钼涂层的平台石墨管中直接进样测定葡萄酒中的铝含量.研究了石墨炉各主要工作条件对吸光度的影响,确定了该方法的最佳条件:0-100μg/L范围内呈线性关系;仪器的检出限为1.7μg/L;应用此方法测定了几种不同样品中铝含量,测定值的相对标准偏差(n=10)在2.28%-3...     

碳化铝与水反应合成甲烷水合物的实验研究

 利用自行设计的高压气水合物实验装置,通过碳化铝与水反应成功合成了甲烷水合物。实验结果表明,碳化铝与水反应合成甲烷水合物的方法有效地解决了传统甲烷水合物模拟实验中甲烷气体引入问题;同时,碳化铝与水反应产生的甲烷及沉淀物能较好地模拟海洋环境中水合物形成的自然条件,为实验模拟甲烷水合物研究提供了一种新方法。利用此方法,对甲烷水合物合成与分解温度、压力条件及动力学过程进行了初步研究。     

CdS/ZnO纳米复合结构的制备、表征及其光催化活性的改善

利用简单的水热法在ZnO纳米棒表面合成CdS纳米粒子.用扫描电镜(SEM)和X射线衍射(XRD)对CdS/ZnO异质结构进行表征.实验结果表明,在生长CdS的过程中ZnO被逐渐地腐蚀.选择CdS/ZnO纳米复合材料作为光催化剂在紫外光和绿光照射的条件下降解甲基橙(MO).CdS/ZnO纳米复合材料纳米棒作为光催化剂降解...     

紫外光固化阳离子复合胶粘剂的制备与表征

 以三芳基六氟磷酸硫鎓盐为引发剂,钛酸四异丙酯(TIP)为无机前驱体,3,4-环氧环己基甲基3,4-环氧环己基甲酸酯为单体,制备了含TiO2纳米结构的紫外光固化阳离子复合胶粘剂。通过原子力显微镜对复合胶粘剂形貌进行表征,研究了TIP含量对胶粘剂折射率和光透过率的影响。结果表明：TiO2无机相均匀地分散在胶粘剂的聚合物基体中,平均粒径约为20 nm;随着体系中TIP质量分数的变化,复合胶粘剂折射率为1.510 3~1.540 9可调;胶粘剂的光透过率随TIP质量分数增加略有减低,但当TIP含量高达40%时,光透过率维持在90%左右。     

引信用激光与加速度传感器复合定高技术

比较了不同类型的弹载定高体制,提出了脉冲激光与重力加速度传感器复合定高的定距原理,并对测距误差进行深入分析,得出其定高精度。对设计出的原理样机进行了实验测试,平台倾斜角度检测实验的结果表明,静态条件下最大角度误差小于0.3;0~500 m定高测试实验的结果表明,测量平均值与实际值最大误差为2.5 m,并且与目标距离无关。     

Neutron diffraction study on composite compound Nd2Co7

The crystallographic and the magnetic structures of the composite compound Nd₂Co₇ at 300 K are investigated by a combined refinement of X-ray diffraction data and high-resolution neutron diffraction data. The compound crystallizes into a hexagonal Ce₂Ni₇-type structure and consists of alternately stacking MgZn₂-type NdCo₂ and CaCu₅-type NdCo₅ structural blocks along the c axis. A magnetic structure model with the moments of all atoms aligning along the c axis provides a satisfactory fitting to the neutron diffraction data and coincides with the easy magnetization direction revealed by the X-ray diffraction experiments on magnetically pre-aligned fine particles. The refinement results show that the derived atomic moments of the Co atoms vary in a range of 0.7 μ_B-1.1 μ_B and the atomic moment of Nd in the NdCo₅ slab is close to the theoretical moment of a free trivalent Nd³⁺ ion, whereas the atomic moment of Nd in the NdCo₂ slab is much smaller than the theoretical value for a free Nd³⁺ ion. The remarkable difference in the atomic moment of Nd atoms between different structural slabs at room temperature is explained in terms of the magnetic characteristics of the NdCo₂ and NdCo₅ compounds and the local chemical environments of the Nd atoms in different structural slabs of the Nd₂Co₇ compound.     

Ti-doped nano-porous graphene: A material for hydrogen storage and sensor

Clustering of Ti on carbon nanostructures has proved to be an obstacle in their use as hydrogen storagematerials. Using density functional theory we show that Ti atoms will not cluster at moderate concentrations when doped into nanoporous graphene. Since each Ti atom can bind up to three hydrogen molecules with an average binding energy of 0.54 eV/H₂, this material can be ideal for storing hydrogen under ambient thermodynamic conditions. In addition, nanoporous graphene is magnetic with or without Ti doping, but when it is fully saturated with hydrogen, the magnetism disappears. This novel feature suggests that nanoporous graphene cannot only be used for storing hydrogen, but also as a hydrogen sensor.