Driving Forces of Protein Diffusion
Diffusivity of a protein (a Brownian particle) is caused by random molecular collisions in the Stokes–Einstein picture. Alternatively, it can be viewed as driven by unbalanced stochastic forces acting from water on the protein. Molecular dynamics simulations of protein mutants carrying different cha...
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Veröffentlicht in: | The journal of physical chemistry letters 2020-12, Vol.11 (23), p.10137-10143 |
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description | Diffusivity of a protein (a Brownian particle) is caused by random molecular collisions in the Stokes–Einstein picture. Alternatively, it can be viewed as driven by unbalanced stochastic forces acting from water on the protein. Molecular dynamics simulations of protein mutants carrying different charges are analyzed here in terms of the van der Waals (vdW) and electrostatic forces acting on the protein. They turn out to be remarkably strongly correlated and the total force is largely a compensation between vdW and electrostatic forces. Both vdW and electrostatic forces relax on the same time scale of 5–6 ns separated by 6 orders of magnitude from the relaxation time of the total force. Similar phenomenology applies to the dynamics and statistics of the fluctuating torque responsible for rotational diffusion. Standard linear theories of dielectric friction are grossly inapplicable to translational and rotational diffusion of proteins overestimating friction by many orders of magnitude. |
doi_str_mv | 10.1021/acs.jpclett.0c03006 |
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Alternatively, it can be viewed as driven by unbalanced stochastic forces acting from water on the protein. Molecular dynamics simulations of protein mutants carrying different charges are analyzed here in terms of the van der Waals (vdW) and electrostatic forces acting on the protein. They turn out to be remarkably strongly correlated and the total force is largely a compensation between vdW and electrostatic forces. Both vdW and electrostatic forces relax on the same time scale of 5–6 ns separated by 6 orders of magnitude from the relaxation time of the total force. Similar phenomenology applies to the dynamics and statistics of the fluctuating torque responsible for rotational diffusion. Standard linear theories of dielectric friction are grossly inapplicable to translational and rotational diffusion of proteins overestimating friction by many orders of magnitude.</description><identifier>ISSN: 1948-7185</identifier><identifier>EISSN: 1948-7185</identifier><identifier>DOI: 10.1021/acs.jpclett.0c03006</identifier><language>eng</language><publisher>American Chemical Society</publisher><subject>Physical Insights into the Biosphere, Atmosphere, and Space</subject><ispartof>The journal of physical chemistry letters, 2020-12, Vol.11 (23), p.10137-10143</ispartof><rights>2020 American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a322t-80652b9ad47c4212dc79140f48c64d12824df8c8aebb873a30d6e453060c28343</citedby><cites>FETCH-LOGICAL-a322t-80652b9ad47c4212dc79140f48c64d12824df8c8aebb873a30d6e453060c28343</cites><orcidid>0000-0002-9352-764X</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://pubs.acs.org/doi/pdf/10.1021/acs.jpclett.0c03006$$EPDF$$P50$$Gacs$$H</linktopdf><linktohtml>$$Uhttps://pubs.acs.org/doi/10.1021/acs.jpclett.0c03006$$EHTML$$P50$$Gacs$$H</linktohtml><link.rule.ids>314,776,780,2752,27053,27901,27902,56713,56763</link.rule.ids></links><search><creatorcontrib>Sarhangi, Setare Mostajabi</creatorcontrib><creatorcontrib>Matyushov, Dmitry V</creatorcontrib><title>Driving Forces of Protein Diffusion</title><title>The journal of physical chemistry letters</title><addtitle>J. Phys. Chem. Lett</addtitle><description>Diffusivity of a protein (a Brownian particle) is caused by random molecular collisions in the Stokes–Einstein picture. Alternatively, it can be viewed as driven by unbalanced stochastic forces acting from water on the protein. Molecular dynamics simulations of protein mutants carrying different charges are analyzed here in terms of the van der Waals (vdW) and electrostatic forces acting on the protein. They turn out to be remarkably strongly correlated and the total force is largely a compensation between vdW and electrostatic forces. Both vdW and electrostatic forces relax on the same time scale of 5–6 ns separated by 6 orders of magnitude from the relaxation time of the total force. Similar phenomenology applies to the dynamics and statistics of the fluctuating torque responsible for rotational diffusion. 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Phys. Chem. Lett</addtitle><date>2020-12-03</date><risdate>2020</risdate><volume>11</volume><issue>23</issue><spage>10137</spage><epage>10143</epage><pages>10137-10143</pages><issn>1948-7185</issn><eissn>1948-7185</eissn><abstract>Diffusivity of a protein (a Brownian particle) is caused by random molecular collisions in the Stokes–Einstein picture. Alternatively, it can be viewed as driven by unbalanced stochastic forces acting from water on the protein. Molecular dynamics simulations of protein mutants carrying different charges are analyzed here in terms of the van der Waals (vdW) and electrostatic forces acting on the protein. They turn out to be remarkably strongly correlated and the total force is largely a compensation between vdW and electrostatic forces. Both vdW and electrostatic forces relax on the same time scale of 5–6 ns separated by 6 orders of magnitude from the relaxation time of the total force. Similar phenomenology applies to the dynamics and statistics of the fluctuating torque responsible for rotational diffusion. Standard linear theories of dielectric friction are grossly inapplicable to translational and rotational diffusion of proteins overestimating friction by many orders of magnitude.</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.jpclett.0c03006</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0002-9352-764X</orcidid></addata></record> |
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title | Driving Forces of Protein Diffusion |
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