2018
DOI: 10.1590/0104-6632.20180352s20160276
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Chemical Potentials of Hard-Core Molecules by a Stepwise Insertion Method

Abstract: A molecular simulation algorithm was implemented to calculate chemical potentials of hard-core molecular systems at high densities. The method is based on the Widom particle insertion method and the stepfunction character of free energy variations. The algorithm was evaluated for hard-sphere mixtures at infinite dilution approximation by varying the solute/solvent diameter ratio, for systems with reduced densities from 0.1 to 0.8. The proposed methodology was verified by comparing simulations of trimers dilute… Show more

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Cited by 5 publications
(2 citation statements)
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“…The pH in the reservoir is determined by pH gc = −log 10 [ a H + / c ⊖ ], with the activity of hydronium ions in the reservoir a H + = c H + exp(βμ ex ), where μ ex = μ CS + μ MSA is the excess chemical potential. The nonideality effects due to Coulomb interactions are taken into account at the mean spherical approximation (MSA) level, while the hard core contribution is calculated using the Carnahan–Starling equation of state β μ MSA = λ B ( 1 + 2 κ d κ d 1 ) d 2 κ , .25em β μ CS = 8 η 9 η 2 + 3 η 3 ( 1 η ) 3 where η = π d 3 3 c t , c t = c s + c a is the total concentration of salt and acid, λ B = q 2 /ϵ w k B T = 7.2 Å is the Bjerrum length, and κ = 8 π λ B c t is the inverse Debye length. The surface groups are characterized by p K a = −log 10 [ K a / c ⊖ ], where K a is the acid dissociation constant of surface groups and φ 0 is the mean-field electrostatic potential at the surface titration sites.…”
Section: Theorymentioning
confidence: 99%
“…The pH in the reservoir is determined by pH gc = −log 10 [ a H + / c ⊖ ], with the activity of hydronium ions in the reservoir a H + = c H + exp(βμ ex ), where μ ex = μ CS + μ MSA is the excess chemical potential. The nonideality effects due to Coulomb interactions are taken into account at the mean spherical approximation (MSA) level, while the hard core contribution is calculated using the Carnahan–Starling equation of state β μ MSA = λ B ( 1 + 2 κ d κ d 1 ) d 2 κ , .25em β μ CS = 8 η 9 η 2 + 3 η 3 ( 1 η ) 3 where η = π d 3 3 c t , c t = c s + c a is the total concentration of salt and acid, λ B = q 2 /ϵ w k B T = 7.2 Å is the Bjerrum length, and κ = 8 π λ B c t is the inverse Debye length. The surface groups are characterized by p K a = −log 10 [ K a / c ⊖ ], where K a is the acid dissociation constant of surface groups and φ 0 is the mean-field electrostatic potential at the surface titration sites.…”
Section: Theorymentioning
confidence: 99%
“…, [66][67][68][69] where the volume fraction is η = πd 3 3 c t . The total excess chemical potential of an ion is then µ ex = µ CS + µ M SA .…”
mentioning
confidence: 99%