Literature DB >> 7710478

How does a protein fold?

A Sali1, E Shakhnovich, M Karplus.   

Abstract

The number of all possible conformations of a polypeptide chain is too large to be sampled exhaustively. Nevertheless, protein sequences do fold into unique native states in seconds (the Levinthal paradox). To determine how the Levinthal paradox is resolved, we use a lattice Monte Carlo model in which the global minimum (native state) is known. The necessary and sufficient condition for folding in this model is that the native state be a pronounced global minimum on the potential surface. This guarantees thermodynamic stability of the native state at a temperature where the chain does not get trapped in local minima. Folding starts by a rapid collapse from a random-coil state to a random semi-compact globule. It then proceeds by a slow, rate-determining search through the semi-compact states to find a transition state from which the chain folds rapidly to the native state. The elements of the folding mechanism that lead to the resolution of the Levinthal paradox are the reduced number of conformations that need to be searched in the semi-compact globule (approximately 10(10) versus approximately 10(16) for the random coil) and the existence of many (approximately 10(3)) transition states. The results have evolutionary implications and suggest principles for the folding of real proteins.

Mesh:

Year:  1994        PMID: 7710478     DOI: 10.1038/369248a0

Source DB:  PubMed          Journal:  Nature        ISSN: 0028-0836            Impact factor:   49.962


  183 in total

1.  What is the role of non-native intermediates of beta-lactoglobulin in protein folding?

Authors:  G Chikenji; M Kikuchi
Journal:  Proc Natl Acad Sci U S A       Date:  2000-12-19       Impact factor: 11.205

2.  Conformational propagation with prion-like characteristics in a simple model of protein folding.

Authors:  P M Harrison; H S Chan; S B Prusiner; F E Cohen
Journal:  Protein Sci       Date:  2001-04       Impact factor: 6.725

3.  Hierarchies and logarithmic oscillations in the temporal relaxation patterns of proteins and other complex systems.

Authors:  R Metzler; J Klafter; J Jortner
Journal:  Proc Natl Acad Sci U S A       Date:  1999-09-28       Impact factor: 11.205

4.  A theoretical search for folding/unfolding nuclei in three-dimensional protein structures.

Authors:  O V Galzitskaya; A V Finkelstein
Journal:  Proc Natl Acad Sci U S A       Date:  1999-09-28       Impact factor: 11.205

5.  A polar, solvent-exposed residue can be essential for native protein structure.

Authors:  R B Hill; W F DeGrado
Journal:  Structure       Date:  2000-05-15       Impact factor: 5.006

6.  Investigation of routes and funnels in protein folding by free energy functional methods.

Authors:  S S Plotkin; J N Onuchic
Journal:  Proc Natl Acad Sci U S A       Date:  2000-06-06       Impact factor: 11.205

7.  Protein folding and unfolding on a complex energy landscape.

Authors:  D T Leeson; F Gai; H M Rodriguez; L M Gregoret; R B Dyer
Journal:  Proc Natl Acad Sci U S A       Date:  2000-03-14       Impact factor: 11.205

8.  Folding protein models with a simple hydrophobic energy function: the fundamental importance of monomer inside/outside segregation.

Authors:  A F Pereira De Araújo
Journal:  Proc Natl Acad Sci U S A       Date:  1999-10-26       Impact factor: 11.205

9.  The topomer-sampling model of protein folding.

Authors:  D A Debe; M J Carlson; W A Goddard
Journal:  Proc Natl Acad Sci U S A       Date:  1999-03-16       Impact factor: 11.205

10.  Quench-flow experiments combined with mass spectrometry show apomyoglobin folds through and obligatory intermediate.

Authors:  V Tsui; C Garcia; S Cavagnero; G Siuzdak; H J Dyson; P E Wright
Journal:  Protein Sci       Date:  1999-01       Impact factor: 6.725

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