Force Dependence of Proteins’ Transition State Position and the Bell–Evans Model

Single-molecule force spectroscopy has opened a new field of research in molecular biophysics and biochemistry. Pulling experiments on individual proteins permit us to monitor conformational transitions with high temporal resolution and measure their free energy landscape. The force–extension curves...

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Autores principales: Marc Rico-Pasto, Annamaria Zaltron, Felix Ritort
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Publicado: MDPI AG 2021
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spelling oai:doaj.org-article:60a415672b234cb6b866377221b85b322021-11-25T18:31:48ZForce Dependence of Proteins’ Transition State Position and the Bell–Evans Model10.3390/nano111130232079-4991https://doaj.org/article/60a415672b234cb6b866377221b85b322021-11-01T00:00:00Zhttps://www.mdpi.com/2079-4991/11/11/3023https://doaj.org/toc/2079-4991Single-molecule force spectroscopy has opened a new field of research in molecular biophysics and biochemistry. Pulling experiments on individual proteins permit us to monitor conformational transitions with high temporal resolution and measure their free energy landscape. The force–extension curves of single proteins often present large hysteresis, with unfolding forces that are higher than refolding ones. Therefore, the high energy of the transition state (TS) in these molecules precludes kinetic rates measurements in equilibrium hopping experiments. In irreversible pulling experiments, force-dependent kinetic rates measurements show a systematic discrepancy between the sum of the folding and unfolding TS distances derived by the kinetic Bell–Evans model and the full molecular extension predicted by elastic models. Here, we show that this discrepancy originates from the force-induced movement of TS. Specifically, we investigate the highly kinetically stable protein barnase, using pulling experiments and the Bell–Evans model to characterize the position of its kinetic barrier. Experimental results show that while the TS stays at a roughly constant distance relative to the native state, it shifts with force relative to the unfolded state. Interestingly, a conversion of the protein extension into amino acid units shows that the TS position follows the Leffler–Hammond postulate: the higher the force, the lower the number of unzipped amino acids relative to the native state. The results are compared with the quasi-reversible unfolding–folding of a short DNA hairpin.Marc Rico-PastoAnnamaria ZaltronFelix RitortMDPI AGarticlesingle-molecule force spectroscopyprotein foldingfree-energy landscapeBell–Evans modelChemistryQD1-999ENNanomaterials, Vol 11, Iss 3023, p 3023 (2021)
institution DOAJ
collection DOAJ
language EN
topic single-molecule force spectroscopy
protein folding
free-energy landscape
Bell–Evans model
Chemistry
QD1-999
spellingShingle single-molecule force spectroscopy
protein folding
free-energy landscape
Bell–Evans model
Chemistry
QD1-999
Marc Rico-Pasto
Annamaria Zaltron
Felix Ritort
Force Dependence of Proteins’ Transition State Position and the Bell–Evans Model
description Single-molecule force spectroscopy has opened a new field of research in molecular biophysics and biochemistry. Pulling experiments on individual proteins permit us to monitor conformational transitions with high temporal resolution and measure their free energy landscape. The force–extension curves of single proteins often present large hysteresis, with unfolding forces that are higher than refolding ones. Therefore, the high energy of the transition state (TS) in these molecules precludes kinetic rates measurements in equilibrium hopping experiments. In irreversible pulling experiments, force-dependent kinetic rates measurements show a systematic discrepancy between the sum of the folding and unfolding TS distances derived by the kinetic Bell–Evans model and the full molecular extension predicted by elastic models. Here, we show that this discrepancy originates from the force-induced movement of TS. Specifically, we investigate the highly kinetically stable protein barnase, using pulling experiments and the Bell–Evans model to characterize the position of its kinetic barrier. Experimental results show that while the TS stays at a roughly constant distance relative to the native state, it shifts with force relative to the unfolded state. Interestingly, a conversion of the protein extension into amino acid units shows that the TS position follows the Leffler–Hammond postulate: the higher the force, the lower the number of unzipped amino acids relative to the native state. The results are compared with the quasi-reversible unfolding–folding of a short DNA hairpin.
format article
author Marc Rico-Pasto
Annamaria Zaltron
Felix Ritort
author_facet Marc Rico-Pasto
Annamaria Zaltron
Felix Ritort
author_sort Marc Rico-Pasto
title Force Dependence of Proteins’ Transition State Position and the Bell–Evans Model
title_short Force Dependence of Proteins’ Transition State Position and the Bell–Evans Model
title_full Force Dependence of Proteins’ Transition State Position and the Bell–Evans Model
title_fullStr Force Dependence of Proteins’ Transition State Position and the Bell–Evans Model
title_full_unstemmed Force Dependence of Proteins’ Transition State Position and the Bell–Evans Model
title_sort force dependence of proteins’ transition state position and the bell–evans model
publisher MDPI AG
publishDate 2021
url https://doaj.org/article/60a415672b234cb6b866377221b85b32
work_keys_str_mv AT marcricopasto forcedependenceofproteinstransitionstatepositionandthebellevansmodel
AT annamariazaltron forcedependenceofproteinstransitionstatepositionandthebellevansmodel
AT felixritort forcedependenceofproteinstransitionstatepositionandthebellevansmodel
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