Issue 46, 2025

Prediction of Henry's law constants for CO2 and CH4 in levulinic acid via different Monte Carlo approaches

Abstract

Henry's law constants of CO2 and CH4 in levulinic acid are predicted at 313.15 K and 101.325 kPa. The Widom test particle insertion method (which is based on excess chemical potential computation) in the NPT ensemble via two different Monte Carlo approaches, viz., CBMC and CFCMC, is implemented. GEMC-NVT simulations are performed to calculate Henry's law constants from the slope of the line fitted to the plot of partial pressure of solute (CO2 or CH4) in the vapour phase versus the mole fraction of solute in liquid levulinic acid. Henry's law constants estimated via all three Monte Carlo methods and for both the solutes show good agreement within statistical uncertainties. The negative value of the Gibbs free energy of transfer (ΔGtrans) of CO2 from the vapour to the solvent (levulinic acid) phase suggests a preference of CO2 for liquid levulinic acid over the vapour phase. The solvation number computed from solute–solvent centre-of-mass radial distribution functions (RDFs) shows a higher value for CH4 than CO2, contrary to the trend in Henry's law constant. Therefore, the local environment around the solute molecule is investigated by computing the solute–solvent site–site intermolecular RDFs. The number integral calculated (up to the first minimum) from site–site intermolecular RDFs of the C(CO2)–methyl group of levulinic acid (CH3(1)) is more than that calculated from the CH4–CH3(1) RDF, confirming the higher solubility of CO2 in levulinic acid than CH4.

Graphical abstract: Prediction of Henry's law constants for CO2 and CH4 in levulinic acid via different Monte Carlo approaches

Supplementary files

Article information

Article type
Paper
Submitted
10 Jul 2025
Accepted
14 Oct 2025
First published
16 Oct 2025

Phys. Chem. Chem. Phys., 2025,27, 24734-24746

Prediction of Henry's law constants for CO2 and CH4 in levulinic acid via different Monte Carlo approaches

P. Kapadiya and J. Adhikari, Phys. Chem. Chem. Phys., 2025, 27, 24734 DOI: 10.1039/D5CP02630J

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