Computing free energy hypersurfaces for anisotropic intermolecular associations

dc.contributor.authorStrumpfer, J
dc.contributor.authorNaidoo, Kevin J
dc.date.accessioned2016-08-15T13:40:37Z
dc.date.available2016-08-15T13:40:37Z
dc.date.issued2010
dc.date.updated2016-08-15T11:40:29Z
dc.description.abstractWe previously used an adaptive reaction coordinate force biasing method for calculating the free energy of conformation (Naidoo and Brady, J Am Chem Soc 1999, 121, 2244) and chemical reactions (Rajamani et al., J Comput Chem 2003, 24, 1775) amongst others. Here, we describe a generalized version able to produce free energies in multiple dimensions, descriptively named the free energies from adaptive reaction coordinate forces method. To illustrate it, we describe how we calculate a multidimensional intermolecular orientational free energy, which can be used to investigate complex systems such as protein conformation and liquids. This multidimensional intermolecular free energy W(r, θ1, θ2, ϕ) provides a measure of orientationally dependent interactions that are appropriate for applications in systems that inherently have molecular anisotropic features. It is a highly informative free energy volume, which can be used to parameterize key terms such as the Gay-Berne intermolecular potential in coarse grain simulations. To demonstrate the value of the information gained from the W(r, θ1, θ2, ϕ) hypersurfaces we calculated them for TIP3P, TIP4P, and TIP5P dimer water models in vacuum. A comparison with a commonly used one-dimensional distance free energy profile is made to illustrate the significant increase in configurational information. The W(r) plots show little difference between the three models while the W(r, θ1, θ2, ϕ) hypersurfaces reveal the underlying energetic reasons why these potentials reproduce tetrahedrality in the condensed phase so differently from each.en_ZA
dc.identifierhttp://dx.doi.org/10.1002/jcc.21317
dc.identifier.apacitationStrumpfer, J., & Naidoo, K. J. (2010). Computing free energy hypersurfaces for anisotropic intermolecular associations. <i>Journal of Computational Chemistry</i>, http://hdl.handle.net/11427/21252en_ZA
dc.identifier.chicagocitationStrumpfer, J, and Kevin J Naidoo "Computing free energy hypersurfaces for anisotropic intermolecular associations." <i>Journal of Computational Chemistry</i> (2010) http://hdl.handle.net/11427/21252en_ZA
dc.identifier.citationStrümpfer, J., & Naidoo, K. J. (2010). Computing free energy hypersurfaces for anisotropic intermolecular associations. Journal of computational chemistry, 31(2), 308-316.en_ZA
dc.identifier.issn0192-8651en_ZA
dc.identifier.ris TY - Journal Article AU - Strumpfer, J AU - Naidoo, Kevin J AB - We previously used an adaptive reaction coordinate force biasing method for calculating the free energy of conformation (Naidoo and Brady, J Am Chem Soc 1999, 121, 2244) and chemical reactions (Rajamani et al., J Comput Chem 2003, 24, 1775) amongst others. Here, we describe a generalized version able to produce free energies in multiple dimensions, descriptively named the free energies from adaptive reaction coordinate forces method. To illustrate it, we describe how we calculate a multidimensional intermolecular orientational free energy, which can be used to investigate complex systems such as protein conformation and liquids. This multidimensional intermolecular free energy W(r, θ1, θ2, ϕ) provides a measure of orientationally dependent interactions that are appropriate for applications in systems that inherently have molecular anisotropic features. It is a highly informative free energy volume, which can be used to parameterize key terms such as the Gay-Berne intermolecular potential in coarse grain simulations. To demonstrate the value of the information gained from the W(r, θ1, θ2, ϕ) hypersurfaces we calculated them for TIP3P, TIP4P, and TIP5P dimer water models in vacuum. A comparison with a commonly used one-dimensional distance free energy profile is made to illustrate the significant increase in configurational information. The W(r) plots show little difference between the three models while the W(r, θ1, θ2, ϕ) hypersurfaces reveal the underlying energetic reasons why these potentials reproduce tetrahedrality in the condensed phase so differently from each. DA - 2010 DB - OpenUCT DP - University of Cape Town J1 - Journal of Computational Chemistry LK - https://open.uct.ac.za PB - University of Cape Town PY - 2010 SM - 0192-8651 T1 - Computing free energy hypersurfaces for anisotropic intermolecular associations TI - Computing free energy hypersurfaces for anisotropic intermolecular associations UR - http://hdl.handle.net/11427/21252 ER - en_ZA
dc.identifier.urihttp://hdl.handle.net/11427/21252
dc.identifier.vancouvercitationStrumpfer J, Naidoo KJ. Computing free energy hypersurfaces for anisotropic intermolecular associations. Journal of Computational Chemistry. 2010; http://hdl.handle.net/11427/21252.en_ZA
dc.languageengen_ZA
dc.publisherWileyen_ZA
dc.publisher.institutionUniversity of Cape Town
dc.rightsCreative Commons Attribution-NonCommercial 4.0 International (CC BY-NC 4.0)*
dc.rights.urihttp://creativecommons.org/licenses/by-nc/4.0/en_ZA
dc.sourceJournal of Computational Chemistryen_ZA
dc.source.urihttp://onlinelibrary.wiley.com/journal/10.1002/(ISSN)1096-987X
dc.titleComputing free energy hypersurfaces for anisotropic intermolecular associationsen_ZA
dc.typeJournal Articleen_ZA
uct.type.filetypeText
uct.type.filetypeImage
uct.type.publicationResearchen_ZA
uct.type.resourceArticleen_ZA
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