An experimental setup of laser-induced graphite plasma was built and the spectral characteristics and properties of graphite plasma were studied. From the temporal behavior of graphite plasma, the duration of CN parti...An experimental setup of laser-induced graphite plasma was built and the spectral characteristics and properties of graphite plasma were studied. From the temporal behavior of graphite plasma, the duration of CN partials （B2 ∑＋ →-X2 ∑＋） emission was two times longer than that of atomic carbon, and all intensities reached the maximum during the early stage from 0.2 μs to 0.8 μs. The electron temperature decreased from 11807 K to 8755 K, the vibration temperature decreased from 8973 K to 6472 K, and the rotational temperature decreased from 7288 K to 4491 K with the delay time, respectively. The effect of the laser energy was also studied, and it was found that the thresholds and spectral characteristics of CN molecular and C atomic spectroscopy presented great differences. At lower laser energies, the electron excited temperature, the electron density, the vibrational temperature and rotational temperature of CN partials increased rapidly. At higher laser energies, the increasing of electron excited temperature and electron density slow down, and the vibrational temperature and rotational temperature even trend to saturation due to plasma shielding and dissociation of CN molecules. The relationship among the three kinds of temperatures was Telec〉Tvib〉Trot at the same time. The electron density of the graphite plasma was in the order of 1017 cm-3 and 1018 cm-3.展开更多
采用基底辅助激光诱导击穿光谱技术,以标准油中的Mg、Ti、Ni与Cr为目标元素进行定量分析。选定Mg II 279.55 nm、Ti I 334.94 nm、Ni I 352.45 nm与Cr I 425.44 nm为目标元素的定量分析谱线进行分析。考察样品预处理静置时间、样品油膜...采用基底辅助激光诱导击穿光谱技术,以标准油中的Mg、Ti、Ni与Cr为目标元素进行定量分析。选定Mg II 279.55 nm、Ti I 334.94 nm、Ni I 352.45 nm与Cr I 425.44 nm为目标元素的定量分析谱线进行分析。考察样品预处理静置时间、样品油膜平均厚度、探测延时和激光脉冲能量对Mg、Ti、Ni与Cr元素光谱信号强度与信背比的影响。在最优的实验条件下,利用6个标准油样品建立了标准曲线定标模型,得出Mg、Ti、Ni与Cr的检出限分别为3.10,8.17,18.79,6.10μg·g^-1。基于定标曲线,预测了另外5个标准油样品中Mg、Ti、Ni与Cr的质量比,相对误差分别为7.43%、8.91%、13.66%与10.40%。展开更多
基金supported by National Natural Science Foundation of China(No.61205149)Scientific Research Foundation for the Returned Overseas Chinese Scholars of State Education Ministry,Science Research Funds of Chongqing Municipal Education Commission(KJ1500436)+2 种基金Scientific and Technological Talents Training Project of Chongqing(CSTC2013kjrc-qnrc40002)Key Project of Foundation and Advanced Technology Research Project of Chongqing(CSTC2015jcyj B0358)Visiting Scholarship of State Key Laboratory of Power Transmission Equipment & System Security and New Technology(2007DA10512714409)
文摘An experimental setup of laser-induced graphite plasma was built and the spectral characteristics and properties of graphite plasma were studied. From the temporal behavior of graphite plasma, the duration of CN partials （B2 ∑＋ →-X2 ∑＋） emission was two times longer than that of atomic carbon, and all intensities reached the maximum during the early stage from 0.2 μs to 0.8 μs. The electron temperature decreased from 11807 K to 8755 K, the vibration temperature decreased from 8973 K to 6472 K, and the rotational temperature decreased from 7288 K to 4491 K with the delay time, respectively. The effect of the laser energy was also studied, and it was found that the thresholds and spectral characteristics of CN molecular and C atomic spectroscopy presented great differences. At lower laser energies, the electron excited temperature, the electron density, the vibrational temperature and rotational temperature of CN partials increased rapidly. At higher laser energies, the increasing of electron excited temperature and electron density slow down, and the vibrational temperature and rotational temperature even trend to saturation due to plasma shielding and dissociation of CN molecules. The relationship among the three kinds of temperatures was Telec〉Tvib〉Trot at the same time. The electron density of the graphite plasma was in the order of 1017 cm-3 and 1018 cm-3.
文摘采用基底辅助激光诱导击穿光谱技术,以标准油中的Mg、Ti、Ni与Cr为目标元素进行定量分析。选定Mg II 279.55 nm、Ti I 334.94 nm、Ni I 352.45 nm与Cr I 425.44 nm为目标元素的定量分析谱线进行分析。考察样品预处理静置时间、样品油膜平均厚度、探测延时和激光脉冲能量对Mg、Ti、Ni与Cr元素光谱信号强度与信背比的影响。在最优的实验条件下,利用6个标准油样品建立了标准曲线定标模型,得出Mg、Ti、Ni与Cr的检出限分别为3.10,8.17,18.79,6.10μg·g^-1。基于定标曲线,预测了另外5个标准油样品中Mg、Ti、Ni与Cr的质量比,相对误差分别为7.43%、8.91%、13.66%与10.40%。
