原子吸收光谱法测定拉伸断口铬镍钼钛钢样品中主成分

研究了毫克级铬镍钼风样品中主成分镍的火焰原子吸收光谱法（FAAS法）和铬、钼、钒、钛、铝的塞曼恒温平台石墨炉原子吸收光谱法（ZSTPF－AAS法）。采用了微波溶样技术作为防污染样品预处理技术，采用石墨管硅涂层改进技术提高了仪器的测试精度。其中铬、镍、钼、钒、钛、铝的相对标准偏差分别为2.7%,0.97%,8.6%,7.3%,1.7%,7.3%。其加标回收率分别为96.5%,97%,96.7%,93%,98%,91%。通过分析，发现在较低温度下铬镍钼钛钢断面上有轻微的钼偏析现象，可能是拉伸断裂的主要化学影响因素。     

热脱附-气相色谱质谱分析热环境下汽车沙发释放的挥发性有机物

汽车沙发部件在热环境中,会释放出许多挥发性有机物(VOC),污染环境,危害人体健康.本研究将汽车沙发放置在2 m3特制塑料采样袋中,在热环境下释放挥发性有机物,然后以Tenax管富集有机物,用热脱附-气相色谱质谱进行分析.结果表明:汽车沙发在热环境状态下,挥发出大量有机物,共定性检测出49种挥发性有机物(VOC),包括...     

对石墨管内锆涂层作用的初探

对石墨管表面进行难熔碳化物涂覆处理,是原子吸收分析中一种操作简单、成本低廉的石墨管改进技术。通常认为,管内的锆涂层可以减少试液及原子蒸气通过管壁的渗透、阻止某些待测元素与管壁直接接触生成难熔碳化物,并可能参与管内的化学反应。我们对涂锆与非涂锆管进行了电子显微形貌观察,并选择锑、锡在涂锆管与非涂锆管中进行了原子吸收测定的对比,以期对试验现象及锆涂层在石墨管内的主要作用做一些初步的探讨。     

原子吸收光谱法测定气样中一氧化碳的研究

本文研究了用自制Ｎｉ（ＣＯ）４发生管和电加热石英管原子化器间接测定一氧化碳的条件，探讨了Ｎｉ（ＣＯ）４的产生和在石英管中原子化效率及干扰消除。     

PVC基管状流通钾离子选择电极的研制及其在流动注射分析中的应用

实验装置由PVC基管状流通钾离子选择电极和与它结合的流动注射分析体系两部分组成。对该体系的分析特点和影响测定的参数进行了讨论,建立了土壤浸提液中钾测定方法,样品分析结果和火焰光度法有良好一致性。     

硒吩聚合物/寡聚物有机光电材料研究进展

主要从光电性能角度总结了近几年硒吩聚合物/寡聚物在有机太阳能电池(OSCs)、场效应晶体管(FETs)、发光二级管(LED)等方面的研究进展。目前,基于聚硒吩并[3,4-b]硒吩-苯并二硒吩(PSeB2)(polyselenopheno[3,4-b]selenophene-co-benzodiselenophene)本体异质结太阳能电池器件的能量转化效率最高,达6.87%;场效应晶体管方面,基于PSeDPP(P28)器件的空穴迁移率最高达1.62cm2.V-1.s-1。基于PFO-DDSTQ(一种硒吩芴基聚合物)的发光二级管,表现出目前基于硒吩化合物的最长波长发光器件,EL光谱峰值约860nm。通过对研究者的研究成果的总结发现,在有机光电器件的应用领域中硒吩聚合物/寡聚物是一种极具应用前景的材料。     

煤油裂解产物/空气与煤油/空气在宽温度范围内点火延迟的对比研究

Kerosene is an ideal endothermic hydrocarbon. Its pyrolysis plays a significant role in the thermal protection for high-speed aircraft. Before it reacts, kerosene experiences thermal decomposition in the heat exchanger and produces cracked products. Thus, to use cracked kerosene instead of pure kerosene, knowledge of their ignition properties is needed. In this study, ignition delay times of cracked kerosene/air and kerosene/air were measured in a heated shock tube at temperatures of 657–1333 K, an equivalence ratio of 1.0, and pressures of 1.01 × 10⁵–10.10 × 10⁵ Pa. Ignition delay time was defined as the time interval between the arrival of the reflected shock and the occurrence of the steepest rise of excited-state CH species (CH*) emission at the sidewall measurement location. Pure helium was used as the driver gas for high-temperature measurements in which test times needed to be shorter than 1.5 ms, and tailored mixtures of He/Ar were used when test times could reach up to 15 ms. Arrhenius-type formulas for the relationship between ignition delay time and ignition conditions (temperature and pressure) were obtained by correlating the measured high-temperature data of both fuels. The results reveal that the ignition delay times of both fuels are close, and an increase in the pressure or temperature causes a decrease in the ignition delay time in the high-temperature region (> 1000 K). Both fuels exhibit similar high-temperature ignition delay properties, because they have close pressure exponents (cracked kerosene: τ_ign∝P^-0.85; kerosene:τ_ign∝P^-0.83) and global activation energies (cracked kerosene: E_a = 143.37 kJ·mol^-1; kerosene: E_a = 144.29 kJ·mol^-1). However, in the low-temperature region (< 1000 K), ignition delay characteristics are quite different. For cracked kerosene/air, while the decrease in the temperature still results in an increase in the ignition delay time, the negative temperature coefficient (NTC) of ignition delay does not occur, and the low-temperature ignition data still can be correlated by an Arrhenius-type formula with a much smaller global activation energy compared to that at high temperatures. However, for kerosene/air, this NTC phenomenon was observed, and the Arrhenius-type formula fails to correlate its low-temperature ignition data. At temperatures ranging from 830 to 1000 K, the cracked kerosene ignites faster than the kerosene; at temperatures below 830 K, kerosene ignition delay times become much shorter than those of cracked kerosene. Surrogates for cracked kerosene and kerosene are proposed based on the H/C ratio and average molecular weight in order to simulate ignition delay times for cracked kerosene/air and kerosene/air. The simulation results are in fairly good agreement with current experimental data for the two fuels at high temperatures (> 1000 K). However, in the low-temperature NTC region, the results are in very good agreement with kerosene ignition delay data but disagree with cracked kerosene ignition delay data. The comparison between experimental data and model predictions indicates that refinement of the reaction mechanisms for cracked kerosene and kerosene is needed. These test results are helpful to understand ignition properties of cracked kerosene in developing regenerative cooling technology for high-speed aircraft.     

衬钽管石墨炉原子吸收法测定痕量镓时基体改进剂的研究及应用

提出用钒和铜混合基体改进剂衬钽管石墨炉原子吸收测定镓的方法。衬钽管使镓的灵敏度提高6倍左右,钒和铜混合基体改进剂不仅能进一步提高灵敏度,而且能提高灰化温度,降低原子化温度,增强抗干扰能力。测定 GSD 标准样品中的镓时,不需对样品进行预分离即可直接进行测定,结果与参考值相符。     

热分解法制备Fe_2O_3修饰的TiO_2纳米管阵列及其光电性能研究

为提高TiO_2纳米管阵列(TiO_2-NTs)的可见光活性,通过阳极氧化和热分解法制备了Fe_2O_3纳米粒子修饰的TiO_2纳米管阵列(Fe_2O_3/TiO_2-NTs)。通过扫描电子显微镜(SEM),透射电子显微镜(TEM)和紫外-可见光漫反射光谱(UV-vis DRS)等对产物进行了相关表征,同时测试了产物的光电性能及其光催化降解甲基橙的性能。结果显示,Fe_2O_3/TiO_2-NTs的光电流强度和光催化降解率分别是是TiO_2-NTs的19倍和8.7倍。     

TiO_2纳米管阵列的多重改性及其在超级电容器中应用的最新进展

阳极氧化法制备的TiO_2纳米管阵列因其简单的制备方法、可控的形貌以及环境友好等优点而成为超级电容器领域重点研究的电极材料之一。本文介绍了TiO_2纳米管的多重改性方法,包括引入氧空位、金属或非金属修饰或掺杂、金属化合物(氧化物、氢氧化物、硫化物、氮化物)以及导电聚合物修饰等,以进一步提高TiO_2纳米管的电化学性能。介绍了近年来阳极氧化法制备的TiO_2纳米管阵列在超级电容器中应用的研究进展,为进一步拓展TiO_2纳米管阵列的实际应用提供参考。