ArticleProceedings of the National Academy of Sciences of the United States of America2011
Folding of the Pit1 homeodomain near the speed limit.
Article in Proceedings of the National Academy of Sciences of the United States of America, 2011. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 4 papers.
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The abstract states no effect estimate the extractor could read, or names no intervention and outcome on the map, so this paper lights no cell and moves no belief. It is still indexed, cited and linked below.
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Who cites it
4 citing papers in PubMed, 10 citations in OpenAlex.
- Protein folding mechanism revealed by single-molecule force spectroscopy experiments.Biophysics reports · 2021Article
- When fast is better: protein folding fundamentals and mechanisms from ultrafast approaches.The Biochemical journal · 2016Review
- Direct quantification of the attempt frequency determining the mechanical unfolding of ubiquitin protein.The Journal of biological chemistry · 2011Article
- Malleability of folding intermediates in the homeodomain superfamily.Proceedings of the National Academy of Sciences of the United States of America · 2011Article
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Authors and funding
3 authors at 2 institutions in 1 country.
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Abstract
Current questions in protein folding mechanisms include how fast can a protein fold and are there energy barriers for the folding and unfolding of ultrafast folding proteins? The small 3-helical engrailed homeodomain protein folds in 1.7 μs to form a well-characterized intermediate, which rearranges in 17 μs to native structure. We found that the homologous pituitary-specific transcription factor homeodomain (Pit1) folded in a similar manner, but in two better separated kinetic phases of 2.3 and 46 μs. The greater separation and better fluorescence changes facilitated a detailed kinetic analysis for the ultrafast phase for formation of the intermediate. Its folding rate constant changed little with denaturant concentration or mutation but unfolding was very sensitive to denaturant and energy changes on mutation. The folding rate constant of 3 × 10(5) s(-1) in water decreased with increasing viscosity, and was extrapolated to 4.4 × 10(5) s(-1) at zero viscosity. Thus, the formation of the intermediate was partly rate limited by chain diffusion and partly by an energy barrier to give a very diffuse transition state, which was followed by the formation of structure. Conversely, the unfolding reaction required the near complete disruption of the tertiary structure of the intermediate in a highly cooperative manner, being exquisitely sensitive to individual mutations. The folding is approaching, but has not reached, the downhill-folding scenario of energy landscape theory. Under folding conditions, there is a small energy barrier between the denatured and transition states but a larger barrier between native and transition states.
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