Skip to main page content
U.S. flag

An official website of the United States government

Dot gov

The .gov means it’s official.
Federal government websites often end in .gov or .mil. Before sharing sensitive information, make sure you’re on a federal government site.

Https

The site is secure.
The https:// ensures that you are connecting to the official website and that any information you provide is encrypted and transmitted securely.

Access keys NCBI Homepage MyNCBI Homepage Main Content Main Navigation
Review
. 1999 May 25;96(11):5897-9.
doi: 10.1073/pnas.96.11.5897.

Searching for "downhill scenarios" in protein folding

Affiliations
Review

Searching for "downhill scenarios" in protein folding

W A Eaton. Proc Natl Acad Sci U S A. .
No abstract available

PubMed Disclaimer

Figures

Figure 1
Figure 1
Schematic of one and two-dimensional free energy surfaces. (Left) Free energy as a function of the fraction of native contacts (Q) and the radius of gyration (Rg). This surface has three significant minima, one for an expanded denatured state (DE), one for a compact denatured state (DC), and one for the native state (N). To simplify the brief discussion of this surface the somewhat unrealistic assumption is made that Q is the same for DE and DC, and Rg is the same for DC and N. For this free energy surface Q may be a good reaction coordinate for forming the native state N from DC or DE, and Rg may be a good reaction coordinate for collapse of the expanded denatured state DE to DC or N, but not vice versa. If so, then the kinetics of folding and unfolding, as well as the kinetics of collapse and expansion of the denatured protein, might be described as diffusion on one-dimensional free energy surfaces (Right). One of the major outstanding issues is whether DE has a topology that is near native (assumed for a “molten globule”) or is more nearly a “random globule” with a distribution of topologies, in which case DC should be considered a trap on the free energy surface containing misfolded structures. (Upper Right) Free energy as a function of Q for folding over a barrier (continuous blue curve) and for downhill folding (dotted red curve) in a type 0 scenario in the classification of Bryngelson et al. (9). (Lower Right) Free energy as a function of Rg. Submillisecond time-resolved small-angle x-ray scattering experiments are being performed that hold the promise of resolving these kinetics (L. Pollack, M. W. Tate, N. C. Darnton, J. B. Knight, S. M. Gruner, W.A.E., and R. H. Austin, unpublished work).

Comment on

References

    1. Lansbury P T. Proc Natl Acad Sci USA. 1999;96:3342–3344. - PMC - PubMed
    1. Onuchic J, Luthey-Schulten A, Wolynes P G. Annu Rev Phys Chem. 1997;48:545–600. - PubMed
    1. Mirny L A, Abkevich V I, Shakhnovich E I. Proc Natl Acad Sci USA. 1998;95:4976–4981. - PMC - PubMed
    1. Sabelko J, Ervin J, Gruebele M. Proc Natl Acad Sci USA. 1999;96:6031–6036. - PMC - PubMed
    1. Frauenfelder H, Sligar S G, Wolynes P G. Science. 1991;254:1598–1603. - PubMed

LinkOut - more resources