An EOS for the Lennard-Jones fluid: A virial expansion approach

A large number (>30 000) of Monte Carlo simulations in range of 0.002–1.41 ρ* and T* ≤ 25 (* for reduced, dimensionless) was performed, producing a dense grid of state points for the internal energy U* and pressure p*. The dense grid in ρ* allows the direct integration to obtain the Helmholtz fre...

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Main Author: Matthias Gottschalk
Format: Article
Language:English
Published: AIP Publishing LLC 2019-12-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5119761
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author Matthias Gottschalk
author_facet Matthias Gottschalk
author_sort Matthias Gottschalk
collection DOAJ
description A large number (>30 000) of Monte Carlo simulations in range of 0.002–1.41 ρ* and T* ≤ 25 (* for reduced, dimensionless) was performed, producing a dense grid of state points for the internal energy U* and pressure p*. The dense grid in ρ* allows the direct integration to obtain the Helmholtz free energy F*. The results in U*, p*, and F* were used to fit an equations of state (EOS) for the Lennard-Jones fluid using the virial thermal coefficients B2–B6 taken from the literature and additional empirical coefficients (C7-C16), which correct the errors due to nonconverging behavior of virial thermal coefficients. Those additional coefficients have the same mathematical form as the virial thermal coefficients. The EOS allows an extrapolation to extreme conditions above T* > 100 and ρ* > 2.
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spelling doaj.art-f18914f26a2a4e53859a1882015d17ce2022-12-21T19:18:15ZengAIP Publishing LLCAIP Advances2158-32262019-12-01912125206125206-1110.1063/1.5119761An EOS for the Lennard-Jones fluid: A virial expansion approachMatthias Gottschalk0GFZ German Research Centre for Geosciences, Section 3.6: Chemistry and Physics of Earth Materials, 14473 Potsdam, Telegrafenberg, GermanyA large number (>30 000) of Monte Carlo simulations in range of 0.002–1.41 ρ* and T* ≤ 25 (* for reduced, dimensionless) was performed, producing a dense grid of state points for the internal energy U* and pressure p*. The dense grid in ρ* allows the direct integration to obtain the Helmholtz free energy F*. The results in U*, p*, and F* were used to fit an equations of state (EOS) for the Lennard-Jones fluid using the virial thermal coefficients B2–B6 taken from the literature and additional empirical coefficients (C7-C16), which correct the errors due to nonconverging behavior of virial thermal coefficients. Those additional coefficients have the same mathematical form as the virial thermal coefficients. The EOS allows an extrapolation to extreme conditions above T* > 100 and ρ* > 2.http://dx.doi.org/10.1063/1.5119761
spellingShingle Matthias Gottschalk
An EOS for the Lennard-Jones fluid: A virial expansion approach
AIP Advances
title An EOS for the Lennard-Jones fluid: A virial expansion approach
title_full An EOS for the Lennard-Jones fluid: A virial expansion approach
title_fullStr An EOS for the Lennard-Jones fluid: A virial expansion approach
title_full_unstemmed An EOS for the Lennard-Jones fluid: A virial expansion approach
title_short An EOS for the Lennard-Jones fluid: A virial expansion approach
title_sort eos for the lennard jones fluid a virial expansion approach
url http://dx.doi.org/10.1063/1.5119761
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