Effects of lengthscales and attractions on the collapse of hydrophobic polymers in water
We present results from extensive molecular dynamics simulations of collapse transitions of hydrophobic polymers in explicit water focused on understanding effects of lengthscale of the hydrophobic surface and of attractive interactions on folding. Hydrophobic polymers display parabolic, protein-lik...
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Veröffentlicht in: | Proceedings of the National Academy of Sciences - PNAS 2007-01, Vol.104 (3), p.733-738 |
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creator | Athawale, Manoj V Goel, Gaurav Ghosh, Tuhin Truskett, Thomas M Garde, Shekhar |
description | We present results from extensive molecular dynamics simulations of collapse transitions of hydrophobic polymers in explicit water focused on understanding effects of lengthscale of the hydrophobic surface and of attractive interactions on folding. Hydrophobic polymers display parabolic, protein-like, temperature-dependent free energy of unfolding. Folded states of small attractive polymers are marginally stable at 300 K and can be unfolded by heating or cooling. Increasing the lengthscale or decreasing the polymer-water attractions stabilizes folded states significantly, the former dominated by the hydration contribution. That hydration contribution can be described by the surface tension model, ΔG = γ(T)ΔA, where the surface tension, γ, is lengthscale-dependent and decreases monotonically with temperature. The resulting variation of the hydration entropy with polymer lengthscale is consistent with theoretical predictions of Huang and Chandler [Huang DM, Chandler D (2000) Proc Natl Acad Sci USA 97:] that explain the blurring of entropy convergence observed in protein folding thermodynamics. Analysis of water structure shows that the polymer-water hydrophobic interface is soft and weakly dewetted, and is characterized by enhanced interfacial density fluctuations. Formation of this interface, which induces polymer folding, is strongly opposed by enthalpy and favored by entropy, similar to the vapor-liquid interface. |
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Hydrophobic polymers display parabolic, protein-like, temperature-dependent free energy of unfolding. Folded states of small attractive polymers are marginally stable at 300 K and can be unfolded by heating or cooling. Increasing the lengthscale or decreasing the polymer-water attractions stabilizes folded states significantly, the former dominated by the hydration contribution. That hydration contribution can be described by the surface tension model, ΔG = γ(T)ΔA, where the surface tension, γ, is lengthscale-dependent and decreases monotonically with temperature. The resulting variation of the hydration entropy with polymer lengthscale is consistent with theoretical predictions of Huang and Chandler [Huang DM, Chandler D (2000) Proc Natl Acad Sci USA 97:] that explain the blurring of entropy convergence observed in protein folding thermodynamics. Analysis of water structure shows that the polymer-water hydrophobic interface is soft and weakly dewetted, and is characterized by enhanced interfacial density fluctuations. 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Hydrophobic polymers display parabolic, protein-like, temperature-dependent free energy of unfolding. Folded states of small attractive polymers are marginally stable at 300 K and can be unfolded by heating or cooling. Increasing the lengthscale or decreasing the polymer-water attractions stabilizes folded states significantly, the former dominated by the hydration contribution. That hydration contribution can be described by the surface tension model, ΔG = γ(T)ΔA, where the surface tension, γ, is lengthscale-dependent and decreases monotonically with temperature. The resulting variation of the hydration entropy with polymer lengthscale is consistent with theoretical predictions of Huang and Chandler [Huang DM, Chandler D (2000) Proc Natl Acad Sci USA 97:] that explain the blurring of entropy convergence observed in protein folding thermodynamics. Analysis of water structure shows that the polymer-water hydrophobic interface is soft and weakly dewetted, and is characterized by enhanced interfacial density fluctuations. Formation of this interface, which induces polymer folding, is strongly opposed by enthalpy and favored by entropy, similar to the vapor-liquid interface.</description><subject>Entropy</subject><subject>Free energy</subject><subject>Hydrophobic and Hydrophilic Interactions</subject><subject>Interfacial tension</subject><subject>Modeling</subject><subject>Molecular biology</subject><subject>Monomers</subject><subject>Physical Sciences</subject><subject>Physics</subject><subject>Polymers</subject><subject>Polymers - chemistry</subject><subject>Protein folding</subject><subject>Simulation</subject><subject>Solutes</subject><subject>Temperature dependence</subject><subject>Thermodynamics</subject><subject>Water - chemistry</subject><issn>0027-8424</issn><issn>1091-6490</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNptkc9rFDEcxYModl09e1JDD96mza9JZi4FKdUKhR604C1kssnOLNlkTDLq_vfNsEu3lQZCDu_zfXxfHgDvMTrDSNDz0at0hjiqMW0xYi_AAqMWV5y16CVYIERE1TDCTsCblDYIobZu0GtwggXBNa3JAvy6stbonGCw0Bm_zn3SypkElV9BlXNUOg_BF93D3Buog3NqTGbm-90qhrEP3aDhGNxua2KCg4d_VTbxLXhllUvm3eFdgruvVz8vr6ub22_fL7_cVLpmJFeYcaGpqgUTTFnMbad5TTuNmW6oFbSpV53teMEIIqqluuO24Vh3DWOmFTVdgou97zh1W7PSxpednRzjsFVxJ4Ma5FPFD71chz8SC85pOUvw-WAQw-_JpCy3Q9KmxPQmTEnypiW4JaSAp_-BmzBFX8JJgjAtt-EFOt9DOoaUorEPm2Ak58rkXJk8VlYmPj4OcOQPHRXgwwGYJ492TFIpngR4Vpd2ci6bf_lotEk5xAeSlCJ4-Y2if9rrVgWp1nFI8u7HHA2VvVvBKL0Hx169JA</recordid><startdate>20070116</startdate><enddate>20070116</enddate><creator>Athawale, Manoj V</creator><creator>Goel, Gaurav</creator><creator>Ghosh, Tuhin</creator><creator>Truskett, Thomas M</creator><creator>Garde, Shekhar</creator><general>National Academy of Sciences</general><general>National Acad Sciences</general><scope>FBQ</scope><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QG</scope><scope>7QL</scope><scope>7QP</scope><scope>7QR</scope><scope>7SN</scope><scope>7SS</scope><scope>7T5</scope><scope>7TK</scope><scope>7TM</scope><scope>7TO</scope><scope>7U9</scope><scope>8FD</scope><scope>C1K</scope><scope>FR3</scope><scope>H94</scope><scope>M7N</scope><scope>P64</scope><scope>RC3</scope><scope>7X8</scope><scope>5PM</scope></search><sort><creationdate>20070116</creationdate><title>Effects of lengthscales and attractions on the collapse of hydrophobic polymers in water</title><author>Athawale, Manoj V ; 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Hydrophobic polymers display parabolic, protein-like, temperature-dependent free energy of unfolding. Folded states of small attractive polymers are marginally stable at 300 K and can be unfolded by heating or cooling. Increasing the lengthscale or decreasing the polymer-water attractions stabilizes folded states significantly, the former dominated by the hydration contribution. That hydration contribution can be described by the surface tension model, ΔG = γ(T)ΔA, where the surface tension, γ, is lengthscale-dependent and decreases monotonically with temperature. The resulting variation of the hydration entropy with polymer lengthscale is consistent with theoretical predictions of Huang and Chandler [Huang DM, Chandler D (2000) Proc Natl Acad Sci USA 97:] that explain the blurring of entropy convergence observed in protein folding thermodynamics. 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subjects | Entropy Free energy Hydrophobic and Hydrophilic Interactions Interfacial tension Modeling Molecular biology Monomers Physical Sciences Physics Polymers Polymers - chemistry Protein folding Simulation Solutes Temperature dependence Thermodynamics Water - chemistry |
title | Effects of lengthscales and attractions on the collapse of hydrophobic polymers in water |
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