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Extending the diffuse layer model of surface acidity behaviour: III. Estimating bound site activity coefficients

机译:扩展表面酸性行为的扩散层模型:III。估计结合位点活性系数

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Although detailed thermodynamic analyses of the 2-pK diffuse layer surface complexation model generally specify bound site activity coefficients for the purpose of accounting for those non-ideal excess free energies contributing to bound site electrochemical potentials, in application these terms are ignored based on one or more of the following assumptions: (1) bound site activity coefficients cancel out in the mass action quotients; (2) bound sites display ideal behaviour; and/or (3) these energies are already included in the exponential Boltzmann terms. In this work it is demonstrated that the bound site charging energy terms discussed in the two previous papers in this series have both conceptual and computational analogies to the charging energy contribution to the activity coefficients obtained from the Debye-Huckel Limiting Law. On high charge density colloidal particles at constant counterion condensation (tau), these charging energies can be related to the surface potential (Psi) by: Delta G(charging) = (1-tau)F Psi (where F is the Faraday constant). If one assumes a maximum practical accuracy of +/-10% in experimental estimates of Psi, then it is suggested that charging energies are likely to be experimentally indiscernible under conditions where tau >= 0.9. These findings support the historical practice of ignoring bound site activity coefficients with the 2-pK diffuse layer surface complexation model in the following situations: for spherical particles with a radius >= 0.1 mu m at ionic strengths >= 0.001M (1 : 1), and for spherical particles with a radius >0.01 mu m at an ionic strength >0.1M (1 : 1). In contrast, charging energies (and non-ideal behaviour) are predicted to be significant at all charge densities and ionic strengths for spherical particles with a radius of 0.001 mu m.
机译:尽管对2-pK扩散层表面络合模型进行详细的热力学分析通常会指定结合位点活度系数,以说明那些有助于结合位点电化学势的非理想过量自由能,但在应用中,这些术语将基于一个或多个忽略以下假设更多:(1)结合位点活动系数在质量作用商中抵消; (2)绑定网站显示理想的行为;和/或(3)这些能量已经包含在指数玻尔兹曼项中。在这项工作中,证明了在该系列的前两篇论文中讨论的约束位点充电能量项在概念上和计算上都类似于充电能量对从Debye-Huckel极限定律获得的活度系数的贡献。在恒定抗衡离子凝结(tau)的高电荷密度胶体粒子上,这些电荷能量可以通过以下方式与表面电势(Psi)相关:ΔG(charge)=(1-tau)F Psi(其中F是法拉第常数) 。如果假设在Psi的实验估计值中最大实际精度为+/- 10%,则表明在tau> = 0.9的条件下,充电能量在实验上可能是无法区分的。这些发现支持以下情况下使用2-pK扩散层表面络合模型忽略结合位点活度系数的历史实践:对于离子强度> = 0.001M(1:1),半径> = 0.1μm的球形颗粒,以及离子强度> 0.1M(1:1),半径> 0.01μm的球形颗粒。相比之下,对于半径为0.001μm的球形颗粒,在所有电荷密度和离子强度下,充电能量(和非理想行为)预计都非常重要。

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