Thermodynamics, statistical mechanics and the vanishing pore width limit of confined fluids

Abstract

Temperature, particle number and volume are the independent variables of the Helmholtz free energy for a bulk fluid. For a fluid confined in a slit pore between two walls, they are usually complemented by the surface area. However, an alternative choice is possible with the volume replaced by the pore width. Although the formulations with such two sets of independent variables are different, we show they are equivalent and present their relations. Corresponding general statistical-mechanics results are also presented. When the pore width becomes very small, the system behaves rather like a two-dimensional (2D) fluid and one can wonder if thermodynamics still holds. We find it remains valid even in the limit of vanishing pore width and show how to treat the divergences in the normal pressure and the chemical potential so that the corresponding 2D results can be obtained. Thus, we show that the Gibbs surface thermodynamics is perfectly capable of describing small systems.

Thermodynamic properties of quasi-one-dimensional fluids

“…In contrast to bulk fluids, the choice of the thermodynamic variables is not unique. 53 There are three volumes: the total volume V = V ∥ V , V ∥ , and V . Here, we adopt the usual choice in computer simulations, i.e., we use V ∥ and V as independent variables, although the latter is not necessarily macroscopic.…”