首页> 外文期刊>Spectrochimica Acta, Part B. Atomic Spectroscopy >Effect of magnesium nitrate vaporization on gas temperature in the graphite furnace
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Effect of magnesium nitrate vaporization on gas temperature in the graphite furnace

机译:硝酸镁汽化对石墨炉气体温度的影响

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The vaporization of magnesium nitrate was observed in longitudinally-heated graphite atomizers, using pyrocoated and Ta-lined tubes and filter furnace, Ar or He as purge gas and 10-200-#mu#g samples. A charge coupled device (CCD) spectrometer and atomic absorption spectrometer were employed to follow the evolution of absorption spectra (200-400 nm), light scattering and emission. Molecular bands of NO and NO_2 were observed below 1000 deg C. Magnesium atomic absorption at 285.2 nm appeared at approximately 1500 deg C in all types of furnaces. The intensity and shape of Mg atomization peak indicated a faster vapor release in pyrocoated than in Ta-lined tubes. Light scattering occurred only in the pyrocoated tube with Ar purge gas. At 1500-1800 deg C it was observed together with Mg absorption using either gas-flow or gas-stop mode. At 2200-2400 deg C the scattering was persistent with gas-stop mode. Light scattering at low temperature showed maximum intensity near the center of the tube axis. Magnesium emission at 382.9 383.2 and 383.8 nm was observed simultaneously with Mg absorption only in the pyrocoated tube, using Ar or He purge gas. The emission lines were identified as Mg ~3P deg - ~3D triplet having 3.24 eV excitation energy. The emitting species were distributed close to the furnace wall. The emitting layer was thinner in He than in Ar. The experimental data show that a radial thermal gradient occurs in the cross section of the pyrocoated tube contemporaneously to the vaporization of MgO. This behavior is attributed to the reaction of the sample vapor with the graphite on the tube wall. The estimated variation of temperature within the cross section of the tube reaches more than 300-400 deg C for 10 #mu#g of magnesium nitrate sampled. The increase of gas temperature above the sample originates a corresponding increase of the vaporization rate. Fast vaporization and thermal gradient together cause the spatial condensation of sample vapor that induces the light scattering.
机译:在纵向加热的石墨雾化器中观察到了硝酸镁的汽化,使用了热镀膜的和Ta衬里的管以及过滤炉,使用Ar或He作为吹扫气体,并使用10-200-μμg样品。电荷耦合器件(CCD)光谱仪和原子吸收光谱仪用于跟踪吸收光谱(200-400 nm),光散射和发射的演变。在低于1000摄氏度时观察到NO和NO_2的分子带。在所有类型的熔炉中,在大约1500摄氏度时出现285.2 nm处的镁原子吸收。 Mg雾化峰的强度和形状表明,热解涂层中的蒸汽释放比Ta衬管中的蒸汽释放更快。光散射仅在使用Ar吹扫气体的热镀管中发生。在1500-1800摄氏度下,使用气流或气体停止模式可以观察到镁的吸收。在2200-2400摄氏度下,以阻气模式持续散射。低温下的光散射在管轴中心附近显示出最大强度。使用Ar或He吹扫气体,仅在热镀膜管中同时观察到382.9 383.2和383.8 nm处的镁发射,同时只有Mg吸收。发射线被鉴定为具有3.24eV激发能的Mg〜3P deg ~~ 3D三重态。排放物分布在靠近炉壁的位置。 He中的发射层比Ar中的发射层薄。实验数据表明,与MgO的蒸发同时,热解管的横截面出现了径向热梯度。该行为归因于样品蒸气与管壁上的石墨的反应。对于10μμg的硝酸镁,在管的横截面内的估计温度变化达到300-400℃以上。样品上方的气体温度升高导致相应的汽化速率升高。快速蒸发和热梯度共同导致样品蒸汽的空间凝结,从而引起光散射。

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