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Free Energy Landscape of the Complete Transport Cycle in a Key Bacterial Transporter
[Image: see text] PepT(So) is a proton-coupled bacterial symporter, from the major facilitator superfamily (MFS), which transports di-/tripeptide molecules. The recently obtained crystal structure of PepT(So) provides an unprecedented opportunity to gain an understanding of functional insights of th...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2018
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6161048/ https://www.ncbi.nlm.nih.gov/pubmed/30276247 http://dx.doi.org/10.1021/acscentsci.8b00330 |
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author | Selvam, Balaji Mittal, Shriyaa Shukla, Diwakar |
author_facet | Selvam, Balaji Mittal, Shriyaa Shukla, Diwakar |
author_sort | Selvam, Balaji |
collection | PubMed |
description | [Image: see text] PepT(So) is a proton-coupled bacterial symporter, from the major facilitator superfamily (MFS), which transports di-/tripeptide molecules. The recently obtained crystal structure of PepT(So) provides an unprecedented opportunity to gain an understanding of functional insights of the substrate transport mechanism. Binding of the proton and peptide molecule induces conformational changes into occluded (OC) and outward-facing (OF) states, which we are able to characterize using molecular dynamics (MD) simulations. The structural knowledge of the OC and OF state is important to fully understand the major energy barrier associated with the transport cycle. In order to gain functional insight into the interstate dynamics, we performed extensive all atom MD simulations. The Markov state model was constructed to identify the free energy barriers between the states, and kinetic information on intermediate pathways was obtained using the transition pathway theory (TPT). TPT shows that the OF state is obtained by the movement of TM1 and TM7 at the extracellular side approximately 12–16 Å away from each other, and the inward movement of TM4 and TM10 at the intracellular halves to 3–4 Å characterizes the OC state. Helix distance distributions obtained from MD simulations were compared with experimental double electron–electron resonance spectroscopy and were found to be in excellent agreement with previous studies. We also predicted the optimal positions for placement of methane thiosulfonate spin label probes to capture the slowest protein dynamics. Our finding sheds light on the conformational cycle of this key membrane transporter and the functional relationships between the multiple intermediate states. |
format | Online Article Text |
id | pubmed-6161048 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2018 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-61610482018-10-01 Free Energy Landscape of the Complete Transport Cycle in a Key Bacterial Transporter Selvam, Balaji Mittal, Shriyaa Shukla, Diwakar ACS Cent Sci [Image: see text] PepT(So) is a proton-coupled bacterial symporter, from the major facilitator superfamily (MFS), which transports di-/tripeptide molecules. The recently obtained crystal structure of PepT(So) provides an unprecedented opportunity to gain an understanding of functional insights of the substrate transport mechanism. Binding of the proton and peptide molecule induces conformational changes into occluded (OC) and outward-facing (OF) states, which we are able to characterize using molecular dynamics (MD) simulations. The structural knowledge of the OC and OF state is important to fully understand the major energy barrier associated with the transport cycle. In order to gain functional insight into the interstate dynamics, we performed extensive all atom MD simulations. The Markov state model was constructed to identify the free energy barriers between the states, and kinetic information on intermediate pathways was obtained using the transition pathway theory (TPT). TPT shows that the OF state is obtained by the movement of TM1 and TM7 at the extracellular side approximately 12–16 Å away from each other, and the inward movement of TM4 and TM10 at the intracellular halves to 3–4 Å characterizes the OC state. Helix distance distributions obtained from MD simulations were compared with experimental double electron–electron resonance spectroscopy and were found to be in excellent agreement with previous studies. We also predicted the optimal positions for placement of methane thiosulfonate spin label probes to capture the slowest protein dynamics. Our finding sheds light on the conformational cycle of this key membrane transporter and the functional relationships between the multiple intermediate states. American Chemical Society 2018-08-28 2018-09-26 /pmc/articles/PMC6161048/ /pubmed/30276247 http://dx.doi.org/10.1021/acscentsci.8b00330 Text en Copyright © 2018 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes. |
spellingShingle | Selvam, Balaji Mittal, Shriyaa Shukla, Diwakar Free Energy Landscape of the Complete Transport Cycle in a Key Bacterial Transporter |
title | Free Energy Landscape of the Complete Transport Cycle
in a Key Bacterial Transporter |
title_full | Free Energy Landscape of the Complete Transport Cycle
in a Key Bacterial Transporter |
title_fullStr | Free Energy Landscape of the Complete Transport Cycle
in a Key Bacterial Transporter |
title_full_unstemmed | Free Energy Landscape of the Complete Transport Cycle
in a Key Bacterial Transporter |
title_short | Free Energy Landscape of the Complete Transport Cycle
in a Key Bacterial Transporter |
title_sort | free energy landscape of the complete transport cycle
in a key bacterial transporter |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6161048/ https://www.ncbi.nlm.nih.gov/pubmed/30276247 http://dx.doi.org/10.1021/acscentsci.8b00330 |
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