School of Chemical Engineering, University of Queensland, St. Lucia, Queensland 4072, Australia.
Langmuir. 2011 Dec 6;27(23):14290-9. doi: 10.1021/la203531j. Epub 2011 Nov 7.
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.
我们提出了计算吸附微分和积分焓变的方程,以便在蒙特卡罗模拟中使用。在外势能作用下,N 个分子的吸附被视为将这些分子从参考气相(状态 1)转移到相同温度和平衡压力(相同化学势)下的吸附系统(状态 2)的一种方式。吸附的过剩量是 N 与假想的气体量之间的差值,该假想气体量占据了系统的可及体积,其密度与参考气体相同。焓变是一个状态函数,它被定义为状态 2 和状态 1 的焓之差,等比热被定义为这个焓变随吸附过剩量的导数的负值。它适合于确定在亚临界条件下,过剩相吸附的微分增量下系统的行为。对于超临界条件,建议使用每个粒子的积分吸附焓,因为在最大过剩浓度处等比热变为无穷大。通过这些明确的定义,我们推导出了适用于一般吸附情况的方程,并展示了如何在蒙特卡罗模拟中使用这些方程。我们将新方程应用于不同温度下的氩气在石墨表面上的吸附,以说明需要使用正确的方程来描述吸附等比热。