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Effect of Anode Dimensions and Location of the t Discharge Gas Inlet Port on the Spatial Distribution of Copper Atoms in a Radio Frequency Glow Discharge Atomizer for Atomic Absorption Spectrometry

机译:原子吸收光谱法用射频辉光放电雾化器中阳极尺寸和t气体进口口位置对铜原子空间分布的影响

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The absorbance of Cu atoms sputtered from a Cu cathode in a laboratory-modified radio frequency glow discharge atomizer for atomic absorption spectrometry was measured at different regions within the atomizer chamber for different discharge parameters. The results show that not only the discharge gas flow rate and pressure but also the applied rf power and the degree of extension of the negative glow have significant effects on the atomization and on the distribution of sputtered atoms within the atomizer chamber. The influence of various diameters and thicknesses of the sampling orifice (anode) on the plasma atomization characteristics and the sample weight loss rates has been examined. By increasing the diameter of the sampling orifice, a larger area of the cathode surface (Cu) was allowed to be sputtered, thereby generating a larger number of atoms (higher absorbance) in the analysis volume, where the sputtered atoms were studied by atomic absorption spectrometry. The absorbance of Cu atoms was inversely related to the thickness of the sampling orifice disk because the distance of the investigated region of the atomizer chamber from the cathode surface increases with increasing thickness of the sampling orifice disk. The rate of sample weight loss was inversely related to the diameter of the sampling orifice at orifice diameters higher than or equal to 4 mm. The rate of sample weight loss as a function of the thickness of the sampling orifice disk indicated that the transport efficiency of the sputtered atoms into the atomizer chamber was higher when a sampling disk having a thickness of 2 mm was used. Changing the location of the discharge gas inlet port resulted in a large increase in the atomic absorption signal. A larger increase in the atomic absorption signal of the sputtered Cu atoms was observed for the modified rf atomizer having the discharge gas inlet port on the body of the sampling orifice disk than for the unmodified rf atomizer having the discharge gas inlet port on the top of the atomizer chamber.
机译:在用于原子吸收光谱法的实验室修改的射频辉光放电雾化器中,从铜阴极溅射出的铜原子的吸光度在雾化器室内的不同区域针对不同的放电参数进行了测量。结果表明,不仅排气流量和压力,而且所施加的rf功率和负辉光的扩展程度都对雾化和雾化器室内溅射原子的分布有重要影响。考察了采样孔(阳极)的各种直径和厚度对等离子体雾化特性和样品失重率的影响。通过增加采样孔的直径,可以溅射更大面积的阴极表面(Cu),从而在分析体积中生成更大数量的原子(更高的吸收率),其中通过原子吸收研究溅射的原子光谱法。 Cu原子的吸光度与采样孔板的厚度成反比,这是因为雾化室的研究区域到阴极表面的距离随着采样孔板的厚度的增加而增加。在孔口直径大于或等于4 mm时,样品重量损失的比率与采样孔口的直径成反比。样品重量损失率与样品孔盘厚度的关系表明,当使用厚度为2 mm的样品盘时,溅射原子进入雾化室的传输效率更高。改变排气入口的位置导致原子吸收信号大大增加。观察到,在采样孔板主体上具有排气入口的改进型rf雾化器的溅射铜原子的原子吸收信号的增大,比在排气孔顶部具有排气入口的未改进的rf雾化器要大。雾化室。

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