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Phys. Rev. E 65, 041923 (2002) [11 pages]

Geometric and statistical properties of the mean-field hydrophobic-polar model, the large-small model, and real protein sequences

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C. T. Shih1,6, Z. Y. Su1, J. F. Gwan2, B. L. Hao3, C. H. Hsieh1, J. L. Lo4, and H. C. Lee4,5
1National Center for High-Performance Computing, Hsinchu, Taiwan, Republic of China
2Forum Modellierung, Forschungszentrum Jülich, D-52425 Jülich, Germany
3Institute of Theoretical Physics, Academia Sinica, Beijing, China
4Department of Physics and Department of Life Science, National Central University, Chungli, Taiwan, Republic of China
5Department of Physics, Stanford University, Palo Alto, California 94305
6Department of Physics, Tunghai University, Taichung, Taiwan, Republic of China

Received 28 March 2001; revised 17 December 2001; published 11 April 2002

Lattice models, for their coarse-grained nature, are best suited for the study of the “designability problem,” the phenomenon in which most of the about 16 000 proteins of known structure have their native conformations concentrated in a relatively small number of about 500 topological classes of conformations. Here it is shown that on a lattice the most highly designable simulated protein structures are those that have the largest number of surface-core switchbacks. A combination of physical, mathematical, and biological reasons that causes the phenomenon is given. By comparing the most foldable model peptides with protein sequences in the Protein Data Bank, it is shown that whereas different models may yield similar designabilities, predicted foldable peptides will simulate natural proteins only when the model incorporates the correct physics and biology, in this case if the main folding force arises from the differing hydrophobicity of the residues, but does not originate, say, from the steric hindrance effect caused by the differing sizes of the residues.

© 2002 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.65.041923
DOI:
10.1103/PhysRevE.65.041923
PACS:
87.10.+e, 87.15.By