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利用石墨炉原子吸收光谱法通过原子吸收信号的后沿确定气态原子与石墨之间的相互作用机制。

Mechanism of interaction between gaseous atoms and graphite determined from the back edge of atomic absorption signal with graphite furnace atomic absorption spectrometry.

作者信息

Imai Shoji, Sasada Chisato, Yamamoto Yuhei

机构信息

Department of Natural Science, Graduate School of Technology, Industrial and Social Sciences, Tokushima University, 2-1 Minamijosanjima, Tokushima, 770-8506, Japan.

Department of Chemistry, Faculty of Science and Technology, Tokushima University, 1-1 Minamijosanjima, Tokushima, 770-8502, Japan.

出版信息

Anal Sci. 2025 Sep;41(9):1491-1499. doi: 10.1007/s44211-025-00809-6. Epub 2025 Jun 18.

Abstract

The energetics of interactions between gaseous atoms and pyorolytic graphite (PG) were investigated by the Gibbs free energy change (ΔG) determined from the back edge of atomic absorption (AA) signa. The Gibbs free energy was estimated by assuming an equilibrium state among the interactions between an analyte atom (M) and a PG surface. Because of its poor reactivity, lead was used as a standard to define a ΔG value of Zero to calculate the loss rate of a hypothetical M without interactions. The kinetic parameters for M were calculated using a diffusion loss model. The ratio of the experimental loss rate to the hypothetical loss rate was used to determine the equilibrium constant (K) for the interaction between M and the PG surface, from which ΔG was calculated. The slope of a linear relationship of ΔG vs. the activation energy (E) of atomization for individual atoms on the PG surface was consistent with that of ΔG vs. the binding energy of adatoms with graphene. It was proposed that the interaction between M and the PG surface was caused by the binding to sites of top-C for Au, C-C bridge for Ag and Pb, a hexagonal hole of sixfold sites within C-ring for Co, Fe and Ni, a pair of terminal-C on zigzag edge for Cr, top-subedge for Mn, and active sites in adjacent graphite layers controlling intercalation for Cu.

摘要

通过由原子吸收(AA)信号的后沿确定的吉布斯自由能变化(ΔG),研究了气态原子与热解石墨(PG)之间相互作用的能量学。通过假设分析物原子(M)与PG表面之间的相互作用处于平衡状态来估算吉布斯自由能。由于铅的反应活性较差,因此将其用作标准来定义ΔG值为零,以计算无相互作用时假设的M的损失率。使用扩散损失模型计算M的动力学参数。实验损失率与假设损失率的比值用于确定M与PG表面之间相互作用的平衡常数(K),并由此计算出ΔG。PG表面上单个原子的ΔG与原子化活化能(E)的线性关系斜率,与ΔG与吸附原子与石墨烯结合能的线性关系斜率一致。有人提出,M与PG表面之间的相互作用是由以下原因引起的:对于金,是与顶部C位点结合;对于银和铅,是与C-C桥结合;对于钴、铁和镍,是与C环内六重位点的六边形孔结合;对于铬,是与锯齿边缘上的一对末端C结合;对于锰,是与顶部亚边缘结合;对于铜,是与控制嵌入的相邻石墨层中的活性位点结合。

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