{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,11,1]],"date-time":"2026-11-01T04:07:57Z","timestamp":1793506077075,"version":"4.5.0"},"reference-count":39,"publisher":"National Academy of Sciences","issue":"19","content-domain":{"domain":["www.pnas.org"],"crossmark-restriction":true},"short-container-title":["Proc. Natl. Acad. Sci. U.S.A."],"published-print":{"date-parts":[[2010,5,11]]},"abstract":"<jats:p>\n                    Protein folding mechanisms are probed experimentally using single-point mutant perturbations. The relative effects on the folding (\n                    <jats:italic>\u03d5<\/jats:italic>\n                    -values) and unfolding (1\u00a0-\u00a0\n                    <jats:italic>\u03d5<\/jats:italic>\n                    ) rates are used to infer the detailed structure of the transition-state ensemble (TSE). Here we analyze kinetic data on &gt;\u00a0800 mutations carried out for 24 proteins with simple kinetic behavior. We find two surprising results: (\n                    <jats:italic>i<\/jats:italic>\n                    ) all mutant effects are described by the equation:\n                    <jats:inline-formula>\n                      <jats:inline-graphic xmlns:xlink=\"http:\/\/www.w3.org\/1999\/xlink\" xlink:href=\"pnas.1000988107eq1.gif\"\/>\n                    <\/jats:inline-formula>\n                    . Therefore all data are consistent with a single\n                    <jats:italic>\u03d5<\/jats:italic>\n                    -value (0.24) with accuracy comparable to experimental precision, suggesting that the structural information in conventional\n                    <jats:italic>\u03d5<\/jats:italic>\n                    -values is low. (\n                    <jats:italic>ii<\/jats:italic>\n                    )\n                    <jats:italic>\u03d5<\/jats:italic>\n                    -values change with stability, increasing in mean value and spread from native to unfolding conditions, and thus cannot be interpreted without proper normalization. We eliminate stability effects calculating the\n                    <jats:italic>\u03d5<\/jats:italic>\n                    -values at the mutant denaturation midpoints; i.e., conditions of zero stability (\n                    <jats:italic>\u03d5<\/jats:italic>\n                    <jats:sup>0<\/jats:sup>\n                    ). We then show that the intrinsic variability is\n                    <jats:italic>\u03d5<\/jats:italic>\n                    <jats:sup>0<\/jats:sup>\n                    \u00a0=\u00a00.36\u00a0\u00b1\u00a00.11, being somewhat larger for \u03b2-sheet-rich proteins than for \u03b1-helical proteins. Importantly, we discover that\n                    <jats:italic>\u03d5<\/jats:italic>\n                    <jats:sup>0<\/jats:sup>\n                    -values are proportional to how many of the residues surrounding the mutated site are local in sequence. High\n                    <jats:italic>\u03d5<\/jats:italic>\n                    <jats:sup>0<\/jats:sup>\n                    -values correspond to protein surface sites, which have few nonlocal neighbors, whereas core residues with many tertiary interactions produce the lowest\n                    <jats:italic>\u03d5<\/jats:italic>\n                    <jats:sup>0<\/jats:sup>\n                    -values. These results suggest a general mechanism in which the TSE at zero stability is a broad conformational ensemble stabilized by local interactions and without specific tertiary interactions, reconciling\n                    <jats:italic>\u03d5<\/jats:italic>\n                    -values with many other empirical observations.\n                  <\/jats:p>","DOI":"10.1073\/pnas.1000988107","type":"journal-article","created":{"date-parts":[[2010,4,23]],"date-time":"2010-04-23T22:26:22Z","timestamp":1272061582000},"page":"8611-8616","update-policy":"https:\/\/doi.org\/10.1073\/pnas.cm10313","source":"Crossref","is-referenced-by-count":105,"title":["Insights into protein folding mechanisms from large scale analysis of mutational effects"],"prefix":"10.1073","volume":"107","author":[{"given":"Athi N.","family":"Naganathan","sequence":"first","affiliation":[{"name":"Centro de Investigaciones Biol\u00f3gicas, Consejo Superior de Investigaciones Cient\u00edficas, Ramiro de Maeztu 9, Madrid 28040, Spain; and"},{"name":"Department of Chemistry &amp; Biochemistry, University of Maryland, College Park, MD 20742"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Victor","family":"Mu\u00f1oz","sequence":"additional","affiliation":[{"name":"Centro de Investigaciones Biol\u00f3gicas, Consejo Superior de Investigaciones Cient\u00edficas, Ramiro de Maeztu 9, Madrid 28040, Spain; and"},{"name":"Department of Chemistry &amp; Biochemistry, University of Maryland, College Park, MD 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