Density functional theory for dense nematic liquid crystals with steric interactions

The celebrated work of Onsager on hard particle systems, based on the truncated second order virial expansion, is valid at relatively low volume fractions for large aspect ratio particles. While it predicts the isotropic-nematic phase transition, it does not provide a realistic equation of state in...

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Huvudupphovsmän: Nascimento, E, Palffy-Muhoray, P, Taylor, J, Virga, E, Zheng, X
Materialtyp: Journal article
Publicerad: American Physical Society 2017
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author Nascimento, E
Palffy-Muhoray, P
Taylor, J
Virga, E
Zheng, X
author_facet Nascimento, E
Palffy-Muhoray, P
Taylor, J
Virga, E
Zheng, X
author_sort Nascimento, E
collection OXFORD
description The celebrated work of Onsager on hard particle systems, based on the truncated second order virial expansion, is valid at relatively low volume fractions for large aspect ratio particles. While it predicts the isotropic-nematic phase transition, it does not provide a realistic equation of state in that the pressure remains finite for arbitrarily high densities. In this work, we derive a mean field density functional form of the Helmholtz free energy for nematics with hard core repulsion. In addition to predicting the isotropic-nematic transition, the model provides a more realistic equation of state. The energy landscape is much richer, and the orientational probability distribution function in the nematic phase possesses a unique feature—it vanishes on a nonzero measure set in orientation space.
first_indexed 2024-03-07T02:17:35Z
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publisher American Physical Society
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spelling oxford-uuid:a2cb0e92-bad3-40c3-a31d-6111e81be2b92022-03-27T02:22:25ZDensity functional theory for dense nematic liquid crystals with steric interactionsJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:a2cb0e92-bad3-40c3-a31d-6111e81be2b9Symplectic Elements at OxfordAmerican Physical Society2017Nascimento, EPalffy-Muhoray, PTaylor, JVirga, EZheng, XThe celebrated work of Onsager on hard particle systems, based on the truncated second order virial expansion, is valid at relatively low volume fractions for large aspect ratio particles. While it predicts the isotropic-nematic phase transition, it does not provide a realistic equation of state in that the pressure remains finite for arbitrarily high densities. In this work, we derive a mean field density functional form of the Helmholtz free energy for nematics with hard core repulsion. In addition to predicting the isotropic-nematic transition, the model provides a more realistic equation of state. The energy landscape is much richer, and the orientational probability distribution function in the nematic phase possesses a unique feature—it vanishes on a nonzero measure set in orientation space.
spellingShingle Nascimento, E
Palffy-Muhoray, P
Taylor, J
Virga, E
Zheng, X
Density functional theory for dense nematic liquid crystals with steric interactions
title Density functional theory for dense nematic liquid crystals with steric interactions
title_full Density functional theory for dense nematic liquid crystals with steric interactions
title_fullStr Density functional theory for dense nematic liquid crystals with steric interactions
title_full_unstemmed Density functional theory for dense nematic liquid crystals with steric interactions
title_short Density functional theory for dense nematic liquid crystals with steric interactions
title_sort density functional theory for dense nematic liquid crystals with steric interactions
work_keys_str_mv AT nascimentoe densityfunctionaltheoryfordensenematicliquidcrystalswithstericinteractions
AT palffymuhorayp densityfunctionaltheoryfordensenematicliquidcrystalswithstericinteractions
AT taylorj densityfunctionaltheoryfordensenematicliquidcrystalswithstericinteractions
AT virgae densityfunctionaltheoryfordensenematicliquidcrystalswithstericinteractions
AT zhengx densityfunctionaltheoryfordensenematicliquidcrystalswithstericinteractions