dc.creatorLi, Peng
dc.creatorOliva, Fabiana Yolanda
dc.creatorNaganathan, Athi N.
dc.creatorMuñoz, Victor
dc.date.accessioned2020-09-14T18:52:24Z
dc.date.accessioned2022-10-15T03:27:10Z
dc.date.available2020-09-14T18:52:24Z
dc.date.available2022-10-15T03:27:10Z
dc.date.created2020-09-14T18:52:24Z
dc.date.issued2009-01
dc.identifierLi, Peng; Oliva, Fabiana Yolanda; Naganathan, Athi N.; Muñoz, Victor; Dynamics of one-state downhill protein folding; National Academy of Sciences; Proceedings of the National Academy of Sciences of The United States of America; 106; 1; 1-2009; 103-108
dc.identifier0027-8424
dc.identifierhttp://hdl.handle.net/11336/113961
dc.identifier1091-6490
dc.identifierCONICET Digital
dc.identifierCONICET
dc.identifier.urihttps://repositorioslatinoamericanos.uchile.cl/handle/2250/4339996
dc.description.abstractThe small helical protein BBL has been shown to fold and unfold in the absence of a free energy barrier according to a battery of quantitative criteria in equilibrium experiments, including probe-dependent equilibrium unfolding, complex coupling between denaturing agents, characteristic DSC thermogram, gradual melting of secondary structure, and heterogeneous atom-by-atom unfolding behaviors spanning the entire unfolding process. Here, we present the results of nanosecond T-jump experiments probing backbone structure by IR and end-to-end distance by FRET. The folding dynamics observed with these two probes are both exponential with common relaxation times but have large differences in amplitude following their probe-dependent equilibrium unfolding. The quantitative analysis of amplitude and relaxation time data for both probes shows that BBL folding dynamics are fully consistent with the one-state folding scenario and incompatible with alternative models involving one or several barrier crossing events. At 333 K, the relaxation time for BBL is 1.3 μs, in agreement with previous folding speed limit estimates. However, late folding events at room temperature are an order of magnitude slower (20 μs), indicating a relatively rough underlying energy landscape. Our results in BBL expose the dynamic features of one-state folding and chart the intrinsic time-scales for conformational motions along the folding process. Interestingly, the simple self-averaging folding dynamics of BBL are the exact dynamic properties required in molecular rheostats, thus supporting a biological role for one-state folding.
dc.languageeng
dc.publisherNational Academy of Sciences
dc.relationinfo:eu-repo/semantics/altIdentifier/doi/https://doi.org/10.1073/pnas.0802986106
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://www.pnas.org/content/106/1/103
dc.rightshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.rightsinfo:eu-repo/semantics/restrictedAccess
dc.subjectDOWNHILL FOLDING
dc.subjectFOLDING LANDSCAPE
dc.subjectLANDSCAPE TOPOGRAPHY
dc.subjectPROTEIN DYNAMICS
dc.titleDynamics of one-state downhill protein folding
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:ar-repo/semantics/artículo
dc.typeinfo:eu-repo/semantics/publishedVersion


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