๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Dynamics of the cluster model of protein folding

โœ Scribed by Minoru I. Kanehisa; Tian Yow Tsong


Publisher
Wiley (John Wiley & Sons)
Year
1979
Tongue
English
Weight
785 KB
Volume
18
Category
Article
ISSN
0006-3525

No coin nor oath required. For personal study only.

โœฆ Synopsis


Abstract

The cluster model of protein folding [Kanehisa, M. I. & Tsong, T. Y. (1978) J. Mol. Biol. 124, 177โ€“194] is further investigated for the thermodynamic and kinetic properties of protein foldingโ€“unfolding transitions. A cluster is a locally formed ordered region in the polypeptide chain due to cooperative interactions among residues. In the cluster model a cooperative term is assigned as proportional to the surface area of a globular cluster. This assignment is compared with that for the helixโ€“coil transition of homopolypeptides, where the cooperative term is proportional to the two ends of a linear helical sequence. The dynamics of the cluster model exhibit a slow phase, which is wellโ€separated from other faster phases, because of the cooperative interaction of the macrosystem. This slow phase not only appears within the transition region, but can also persist well below the transition region if the cooperativity depends on the external condition. The amplitudes of certain kinetic phases can vary depending on the choice of physical parameters monitoring the reaction. Thus the same reaction may display different time courses. The qualitative aspects of the folding dynamics are as follows. In one case the rateโ€limiting formation of a criticalโ€size cluster is followed by its rapid growth, while in the other the rateโ€limiting step appears in a later stage, where preformed smaller clusters merge into larger ones. The former case is similar to the dynamics of the helixโ€“coil transition, and the latter represents a stepwise mechanism of protein structure formation.


๐Ÿ“œ SIMILAR VOLUMES


Statistical mechanics of protein folding
โœ Gordon M. Crippen ๐Ÿ“‚ Article ๐Ÿ“… 2004 ๐Ÿ› Wiley (John Wiley & Sons) ๐ŸŒ English โš– 166 KB ๐Ÿ‘ 1 views

## Abstract This is our second type of model for protein folding where the configurational parameters and the effective potential energy function are chosen in such a way that all conformations are described and the canonical partition function can be evaluated analytically. Structure is described

Computer simulations of protein folding
โœ Philippe Ferrara; Joannis Apostolakis; Amedeo Caflisch ๐Ÿ“‚ Article ๐Ÿ“… 2000 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 362 KB ๐Ÿ‘ 3 views

We have performed 128 folding and 45 unfolding molecular dynamics runs of chymotrypsin inhibitor 2 (CI2) with an implicit solvation model for a total simulation time of 0.4 microseconds. Folding requires that the three-dimensional structure of the native state is known. It was simulated at 300 K by

A simple model of chaperonin-mediated pr
โœ Chan, Hue Sun; Dill, Ken A. ๐Ÿ“‚ Article ๐Ÿ“… 1996 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 678 KB

Chaperonins are oligomeric proteins that help other proteins fold. They act, according to the "Anfinsen cage" or "box of infinite dilution" model, to provide private space, protected from aggregation, where a protein can fold. Recent evidence indicates, however, that proteins are often ejected from

A heteropolymer model study for the mech
โœ Masataka Fukugita; David Lancaster; Mark G. Mitchard ๐Ÿ“‚ Article ๐Ÿ“… 1997 ๐Ÿ› Wiley (John Wiley & Sons) ๐ŸŒ English โš– 913 KB

## 4 It('[['r<)[){]l!fn ('r tnodel (d rundoml~.scll~in(eruc[itrgchuirrs /n [MOdimcn.sitms is .studicd Lt'i[h numericul ,sitnulu(ions {n order [C] ehicida(e th(~.ji]ldingmechanism oj protein. H),find (hat the model occasionally . SIMN{ .S,li~lding propen.si[~,depending on [he .wqacnce ()/" random nam