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A van der Waals-type equation of state for fluids with associating molecules

机译:具有缔合分子的流体的范德华型状态方程

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摘要

The basic assumptions of van der Waals theory are contained in two well-known concepts: excluded volume (repulsive forces) and a homogeneous, isotropic field potential (attractive forces). We have superimposed on these, one more well-known concept: the existence of dimers, trimers, etc., at chemical equilibrium. With reasonable simplifying assumptions, we obtain a closed-form equation of state, applicable to all fluid densities, and potentially useful for fluids containing strongly polar or hydrogen-bonded molecules. At all temperatures and at high densities, the equation of state suggests a phase transition where, because of extensive association, a new (solid-like) phase is in equilibrium with a “normal” fluid phase. The boundary between these phases has no critical point.
机译:范德华理论的基本假设包含在两个众所周知的概念中:排除体积(排斥力)和均质的各向同性电场势(吸引力)。我们将这些叠加在一个更广为人知的概念上:在化学平衡状态下二聚体,三聚体等的存在。通过合理的简化假设,我们可以获得适用于所有流体密度的封闭状态方程,该状态方程可能适用于包含强极性或氢键分子的流体。在所有温度和高密度下,状态方程都表明存在一种相变,由于广泛的结合,新的(固态)相与“正常”流体相处于平衡状态。这些阶段之间的边界没有临界点。

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