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Folding Protein Models with a Simple Hydrophobic Energy Function: The Fundamental Importance of Monomer Inside/Outside Segregation
The present study explores a "hydrophobic" energy function for folding simulations of the protein lattice model. The contribution of each monomer to conformational energy is the product of its "hydrophobicity" and the number of contacts it makes, i.e., E($\overset \rightarrow \to...
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Published in: | Proceedings of the National Academy of Sciences - PNAS 1999-10, Vol.96 (22), p.12482-12487 |
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description | The present study explores a "hydrophobic" energy function for folding simulations of the protein lattice model. The contribution of each monomer to conformational energy is the product of its "hydrophobicity" and the number of contacts it makes, i.e., E($\overset \rightarrow \to{\text{h}}$,$\overset \rightarrow \to{\text{c}})$ =-Σ i=1N$\text{c}_{\text{i}}\text{h}_{\text {i}}$ $=-(\overset \rightarrow \to{\text{h}}$.$\overset \rightarrow \to{\text{c}})$ is the negative scalar product between two vectors in N-dimensional cartesian space: $\overset \rightarrow \to{\text{h}}$ =(h1,...,hN) which represents monomer hydrophobicities and is sequence-dependent; and $\overset \rightarrow \to{\text{c}}$ =(c1,...,cN), which represents the number of contacts made by each monomer and is conformation-dependent. A simple theoretical analysis shows that restrictions are imposed concomitantly on both sequences and native structures if the stability criterion for protein-like behavior is to be satisfied. Given a conformation with vector $\overset \rightarrow \to{\text{c}}$, the best sequence is a vector $\overset \rightarrow \to{\text{h}}$ on the direction upon which the projection of $\overset \rightarrow \to{\text{c}}$ - $\overset \rightarrow \to{\overline{\text{c}}}$ is maximal, where $\overset \rightarrow \to{\overline{\text{c}}}$ is the diagonal vector with components equal to $\overline{\text{c}}$, the average number of contacts per monomer in the unfolded state. Best native conformations are suggested to be not maximally compact, as assumed in many studies, but the ones with largest variance of contacts among its monomers, i.e., with monomers tending to occupy completely buried or completely exposed positions. This inside/outside segregation is reflected on an apolar/polar distribution on the corresponding sequence. Monte Carlo simulations in two dimensions corroborate this general scheme. Sequences targeted to conformations with large contact variances folded cooperatively with thermodynamics of a two-state transition. Sequences targeted to maximally compact conformations, which have lower contact variance, were either found to have degenerate ground state or to fold with much lower cooperativity. |
doi_str_mv | 10.1073/pnas.96.22.12482 |
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Pereira de Araújo</creator><creatorcontrib>Antônio F. Pereira de Araújo</creatorcontrib><description>The present study explores a "hydrophobic" energy function for folding simulations of the protein lattice model. The contribution of each monomer to conformational energy is the product of its "hydrophobicity" and the number of contacts it makes, i.e., E($\overset \rightarrow \to{\text{h}}$,$\overset \rightarrow \to{\text{c}})$ =-Σ i=1N$\text{c}_{\text{i}}\text{h}_{\text {i}}$ $=-(\overset \rightarrow \to{\text{h}}$.$\overset \rightarrow \to{\text{c}})$ is the negative scalar product between two vectors in N-dimensional cartesian space: $\overset \rightarrow \to{\text{h}}$ =(h1,...,hN) which represents monomer hydrophobicities and is sequence-dependent; and $\overset \rightarrow \to{\text{c}}$ =(c1,...,cN), which represents the number of contacts made by each monomer and is conformation-dependent. A simple theoretical analysis shows that restrictions are imposed concomitantly on both sequences and native structures if the stability criterion for protein-like behavior is to be satisfied. Given a conformation with vector $\overset \rightarrow \to{\text{c}}$, the best sequence is a vector $\overset \rightarrow \to{\text{h}}$ on the direction upon which the projection of $\overset \rightarrow \to{\text{c}}$ - $\overset \rightarrow \to{\overline{\text{c}}}$ is maximal, where $\overset \rightarrow \to{\overline{\text{c}}}$ is the diagonal vector with components equal to $\overline{\text{c}}$, the average number of contacts per monomer in the unfolded state. Best native conformations are suggested to be not maximally compact, as assumed in many studies, but the ones with largest variance of contacts among its monomers, i.e., with monomers tending to occupy completely buried or completely exposed positions. This inside/outside segregation is reflected on an apolar/polar distribution on the corresponding sequence. Monte Carlo simulations in two dimensions corroborate this general scheme. Sequences targeted to conformations with large contact variances folded cooperatively with thermodynamics of a two-state transition. Sequences targeted to maximally compact conformations, which have lower contact variance, were either found to have degenerate ground state or to fold with much lower cooperativity.</description><identifier>ISSN: 0027-8424</identifier><identifier>EISSN: 1091-6490</identifier><identifier>DOI: 10.1073/pnas.96.22.12482</identifier><identifier>PMID: 10535948</identifier><language>eng</language><publisher>United States: National Academy of Sciences of the United States of America</publisher><subject>Alphabets ; Amino acids ; Biological Sciences ; Energy ; Hydrophobicity ; Mathematical vectors ; Modeling ; Models, Chemical ; Molecular biology ; Monomers ; Monte Carlo Method ; Protein Folding ; Proteins ; Specific heat ; Standard deviation ; Transition temperature</subject><ispartof>Proceedings of the National Academy of Sciences - PNAS, 1999-10, Vol.96 (22), p.12482-12487</ispartof><rights>Copyright 1993-1999 National Academy of Sciences of the United States of America</rights><rights>Copyright National Academy of Sciences Oct 26, 1999</rights><rights>Copyright © 1999, The National Academy of Sciences 1999</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c493t-80a8ca718ea06946bd966e3d02074943126087dd78735faa6e679555a6f2849f3</citedby><cites>FETCH-LOGICAL-c493t-80a8ca718ea06946bd966e3d02074943126087dd78735faa6e679555a6f2849f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://www.pnas.org/content/96/22.cover.gif</thumbnail><linktopdf>$$Uhttps://www.jstor.org/stable/pdf/49373$$EPDF$$P50$$Gjstor$$H</linktopdf><linktohtml>$$Uhttps://www.jstor.org/stable/49373$$EHTML$$P50$$Gjstor$$H</linktohtml><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/10535948$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Antônio F. Pereira de Araújo</creatorcontrib><title>Folding Protein Models with a Simple Hydrophobic Energy Function: The Fundamental Importance of Monomer Inside/Outside Segregation</title><title>Proceedings of the National Academy of Sciences - PNAS</title><addtitle>Proc Natl Acad Sci U S A</addtitle><description>The present study explores a "hydrophobic" energy function for folding simulations of the protein lattice model. The contribution of each monomer to conformational energy is the product of its "hydrophobicity" and the number of contacts it makes, i.e., E($\overset \rightarrow \to{\text{h}}$,$\overset \rightarrow \to{\text{c}})$ =-Σ i=1N$\text{c}_{\text{i}}\text{h}_{\text {i}}$ $=-(\overset \rightarrow \to{\text{h}}$.$\overset \rightarrow \to{\text{c}})$ is the negative scalar product between two vectors in N-dimensional cartesian space: $\overset \rightarrow \to{\text{h}}$ =(h1,...,hN) which represents monomer hydrophobicities and is sequence-dependent; and $\overset \rightarrow \to{\text{c}}$ =(c1,...,cN), which represents the number of contacts made by each monomer and is conformation-dependent. A simple theoretical analysis shows that restrictions are imposed concomitantly on both sequences and native structures if the stability criterion for protein-like behavior is to be satisfied. Given a conformation with vector $\overset \rightarrow \to{\text{c}}$, the best sequence is a vector $\overset \rightarrow \to{\text{h}}$ on the direction upon which the projection of $\overset \rightarrow \to{\text{c}}$ - $\overset \rightarrow \to{\overline{\text{c}}}$ is maximal, where $\overset \rightarrow \to{\overline{\text{c}}}$ is the diagonal vector with components equal to $\overline{\text{c}}$, the average number of contacts per monomer in the unfolded state. Best native conformations are suggested to be not maximally compact, as assumed in many studies, but the ones with largest variance of contacts among its monomers, i.e., with monomers tending to occupy completely buried or completely exposed positions. This inside/outside segregation is reflected on an apolar/polar distribution on the corresponding sequence. Monte Carlo simulations in two dimensions corroborate this general scheme. Sequences targeted to conformations with large contact variances folded cooperatively with thermodynamics of a two-state transition. Sequences targeted to maximally compact conformations, which have lower contact variance, were either found to have degenerate ground state or to fold with much lower cooperativity.</description><subject>Alphabets</subject><subject>Amino acids</subject><subject>Biological Sciences</subject><subject>Energy</subject><subject>Hydrophobicity</subject><subject>Mathematical vectors</subject><subject>Modeling</subject><subject>Models, Chemical</subject><subject>Molecular biology</subject><subject>Monomers</subject><subject>Monte Carlo Method</subject><subject>Protein Folding</subject><subject>Proteins</subject><subject>Specific heat</subject><subject>Standard deviation</subject><subject>Transition temperature</subject><issn>0027-8424</issn><issn>1091-6490</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1999</creationdate><recordtype>article</recordtype><recordid>eNp9kUtv1DAUhSMEokNhj1iA1QVik6lf8QOxqaoOHamoSC1ry5M4Mx4ldmo7wGz55TjMULUsWF1Z9zvH5-oUxWsE5whycjo4HeeSzTGeI0wFflLMEJSoZFTCp8UMQsxLQTE9Kl7EuIUQykrA58URghWpJBWz4tfCd411a_A1-GSsA198Y7oIfti0ARrc2H7oDLjcNcEPG7-yNbhwJqx3YDG6OlnvPoLbjZleje6NS7oDy37wIWlXG-Db7Od8bwJYumgbc3o9pmmCG7MOZq0nh5fFs1Z30bw6zOPi2-Li9vyyvLr-vDw_uyprKkkqBdSi1hwJoyGTlK0ayZghDcSQU0kJwgwK3jRccFK1WjPDuKyqSrMWCypbclx82vsO46o3TZ3TBt2pIdheh53y2qrHG2c3au2_K4xlxbL8_UEe_N1oYlK9jbXpOu2MH6NiEiOCBM3gyT_g1o_B5dMUhojw7MUzBPdQHXyMwbT3ORBUU7dq6lZJln9Xf7rNkrcP8z8Q7MvMwLsDMEn_rh9bfPg_odqx65L5mTL6Zo9uY_Lhns1VcEJ-A3FRwyM</recordid><startdate>19991026</startdate><enddate>19991026</enddate><creator>Antônio F. 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Pereira de Araújo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c493t-80a8ca718ea06946bd966e3d02074943126087dd78735faa6e679555a6f2849f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1999</creationdate><topic>Alphabets</topic><topic>Amino acids</topic><topic>Biological Sciences</topic><topic>Energy</topic><topic>Hydrophobicity</topic><topic>Mathematical vectors</topic><topic>Modeling</topic><topic>Models, Chemical</topic><topic>Molecular biology</topic><topic>Monomers</topic><topic>Monte Carlo Method</topic><topic>Protein Folding</topic><topic>Proteins</topic><topic>Specific heat</topic><topic>Standard deviation</topic><topic>Transition temperature</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Antônio F. 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Pereira de Araújo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Folding Protein Models with a Simple Hydrophobic Energy Function: The Fundamental Importance of Monomer Inside/Outside Segregation</atitle><jtitle>Proceedings of the National Academy of Sciences - PNAS</jtitle><addtitle>Proc Natl Acad Sci U S A</addtitle><date>1999-10-26</date><risdate>1999</risdate><volume>96</volume><issue>22</issue><spage>12482</spage><epage>12487</epage><pages>12482-12487</pages><issn>0027-8424</issn><eissn>1091-6490</eissn><abstract>The present study explores a "hydrophobic" energy function for folding simulations of the protein lattice model. The contribution of each monomer to conformational energy is the product of its "hydrophobicity" and the number of contacts it makes, i.e., E($\overset \rightarrow \to{\text{h}}$,$\overset \rightarrow \to{\text{c}})$ =-Σ i=1N$\text{c}_{\text{i}}\text{h}_{\text {i}}$ $=-(\overset \rightarrow \to{\text{h}}$.$\overset \rightarrow \to{\text{c}})$ is the negative scalar product between two vectors in N-dimensional cartesian space: $\overset \rightarrow \to{\text{h}}$ =(h1,...,hN) which represents monomer hydrophobicities and is sequence-dependent; and $\overset \rightarrow \to{\text{c}}$ =(c1,...,cN), which represents the number of contacts made by each monomer and is conformation-dependent. A simple theoretical analysis shows that restrictions are imposed concomitantly on both sequences and native structures if the stability criterion for protein-like behavior is to be satisfied. Given a conformation with vector $\overset \rightarrow \to{\text{c}}$, the best sequence is a vector $\overset \rightarrow \to{\text{h}}$ on the direction upon which the projection of $\overset \rightarrow \to{\text{c}}$ - $\overset \rightarrow \to{\overline{\text{c}}}$ is maximal, where $\overset \rightarrow \to{\overline{\text{c}}}$ is the diagonal vector with components equal to $\overline{\text{c}}$, the average number of contacts per monomer in the unfolded state. Best native conformations are suggested to be not maximally compact, as assumed in many studies, but the ones with largest variance of contacts among its monomers, i.e., with monomers tending to occupy completely buried or completely exposed positions. This inside/outside segregation is reflected on an apolar/polar distribution on the corresponding sequence. Monte Carlo simulations in two dimensions corroborate this general scheme. Sequences targeted to conformations with large contact variances folded cooperatively with thermodynamics of a two-state transition. Sequences targeted to maximally compact conformations, which have lower contact variance, were either found to have degenerate ground state or to fold with much lower cooperativity.</abstract><cop>United States</cop><pub>National Academy of Sciences of the United States of America</pub><pmid>10535948</pmid><doi>10.1073/pnas.96.22.12482</doi><tpages>6</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Alphabets Amino acids Biological Sciences Energy Hydrophobicity Mathematical vectors Modeling Models, Chemical Molecular biology Monomers Monte Carlo Method Protein Folding Proteins Specific heat Standard deviation Transition temperature |
title | Folding Protein Models with a Simple Hydrophobic Energy Function: The Fundamental Importance of Monomer Inside/Outside Segregation |
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