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首页> 外文期刊>Langmuir: The ACS Journal of Surfaces and Colloids >Development of equations for differential and integral enthalpy change of adsorption for simulation studies
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Development of equations for differential and integral enthalpy change of adsorption for simulation studies

机译:为模拟研究开发吸附微分和积分焓变方程

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We present equations to calculate the differential and integral enthalpy changes of adsorption for their use in Monte Carlo simulation. Adsorption of a system of N molecules, subject to an external potential energy, is viewed as one of transferring these molecules from a reference gas phase (state 1) to the adsorption system (state 2) at the same temperature and equilibrium pressure (same chemical potential). The excess amount adsorbed is the difference between N and the hypothetical amount of gas occupying the accessible volume of the system at the same density as the reference gas. The enthalpy change is a state function, which is defined as the difference between the enthalpies of state 2 and state 1, and the isosteric heat is defined as the negative of the derivative of this enthalpy change with respect to the excess amount of adsorption. It is suitable to determine how the system behaves for a differential increment in the excess phase adsorbed under subcritical conditions. For supercritical conditions, use of the integral enthalpy of adsorption per particle is recommended since the isosteric heat becomes infinite at the maximum excess concentration. With these unambiguous definitions we derive equations which are applicable for a general case of adsorption and demonstrate how they can be used in a Monte Carlo simulation. We apply the new equations to argon adsorption at various temperatures on a graphite surface to illustrate the need to use the correct equation to describe isosteric heat of adsorption.
机译:我们提出方程,以计算吸附的微分和积分焓变化,以用于蒙特卡罗模拟。 N分子系统的吸附受外部势能的影响,被视为在相同温度和平衡压力(相同化学反应)下将这些分子从参考气相(状态1)转移到吸附系统(状态2)中的一种潜在)。吸附的过量量是N和假设的气体量之差,该气体在与参考气体相同的密度下占据系统的可访问体积。焓变化是状态函数,其定义为状态2和状态1的焓之差,等规热定义为该焓变化的导数相对于过量吸附量的负值。确定在亚临界条件下吸附的过量相中系统如何表现出差异增量是合适的。对于超临界条件,建议使用每个粒子的积分吸附焓,因为在最大过量浓度下,等排热变得无限大。通过这些明确的定义,我们得出了适用于一般吸附情况的方程式,并演示了如何在蒙特卡洛模拟中使用它们。我们将新的方程式应用于石墨表面上各种温度下的氩气吸附,以说明需要使用正确的方程式描述吸附的等位线热。

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