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Chemical equilibria of multiple-reaction systems from reaction ensemble Monte Carlo simulation and a predictive equation of state: Combined hydrogenation of ethylene and propylene
Affiliation:1. Laboratory of Thermodynamics in Emerging Technologies, Swiss Federal Institute of Technology, ETH, Zürich, Switzerland;2. Laboratory for I.C. Engines, Empa, Swiss Federal Laboratories for Materials Testing and Research, Dübendorf, Switzerland;3. Ascomp GmbH, Zürich, Switzerland;1. Université de Toulouse, Institut Carnot CIRIMAT, INPT-ENSIACET, 4 allée Emile Monso, BP-44362, 31432 Toulouse Cedex 4, France;2. Air Liquide R&D, Paris-Saclay Research Center, 1 chemin de la porte des loges, BP-126, 78354 Jouy-en-Josas Cedex, France;1. Université de Toulouse, Institut Carnot CIRIMAT, INPT-ENSIACET, 4 allée Emile Monso, CS 44362, 31030 Toulouse Cedex 4, France;2. Materials Science & Technology Division, Oak Ridge National Laboratory, 1 Bethel Valley Road, 37831 Oak Ridge, TN, USA;1. CIRIMAT, Université de Toulouse, CNRS, INPT, UPS, ENSIACET, 4 allée Emile Monso BP 44362, 31030 Toulouse cedex 4, France;2. Air Liquide R&D, Paris-Saclay Research Center, 1 chemin de la porte des loges, BP-126, 78354 Jouy-en-Josas Cedex, France;3. Université de Toulouse, CNRS, Mines Albi, INSA, UPS, ISAE-SUPAERO, ICA (Institut Clément Ader), Campus Jarlard, F-81013 Albi, France
Abstract:Successful application of the reaction ensemble Monte Carlo (REMC) method to compute multiple-reaction chemical equilibria requires a reasonably high acceptance probability for all forward and backward reaction moves during the production stage of a simulation run. To achieve this for a system that involves almost irreversible multiple reactions, it is necessary to choose a thermodynamically-equivalent alternative set of linearly independent reactions, such that the occurrence of very large chemical equilibrium constants is avoided for as many reactions in the set as possible. In this work, the need for such a strategy is justified and applied to the combined hydrogenation of ethylene and propylene, which involves six components and requires a set of four linearly independent reactions. Already validated effective pair potential models were used: one-center Lennard–Jones (1CLJ) models for hydrogen and methane, two-center LJ plus point quadrupole (2CLJQ) models for ethylene, ethane and propylene, and a three-center LJ (3CLJ) model for propane. No binary adjustable parameters were needed to compute the unlike-pair LJ interactions. Simulation results were obtained for the effect of temperature and pressure on the conversions of ethylene and propylene, yield of methane, and density of the system at equilibrium. These results were found to be in very good agreement with calculations using the PSRK group contribution equation of state.
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