| HOME | HELP | FEEDBACK | SUBSCRIPTIONS | ARCHIVE | SEARCH | TABLE OF CONTENTS |

* Department of Chemical Engineering, North Carolina State University, Raleigh, North Carolina 27695-7905; and
Department of Physiology and Biophysics, State University of New York at Buffalo, Buffalo, New York 14214
Correspondence: Address reprint requests to Carol K. Hall, E-mail: hall{at}turbo.che.ncsu.edu.
We have performed discontinuous molecular dynamic simulations of the assembly and folding kinetics of a tetrameric ß-sheet complex that contains four identical four-stranded antiparallel ß-sheet peptides. The potential used in the simulation is a hybrid Go-type potential characterized by the bias gap parameter g, an artificial measure of a model protein's preference for its native state, and the intermolecular contact parameter
, which measures the ratio of intermolecular to intramolecular native attractions. The formation of the ß-sheet complex and its equilibrium properties strongly depend on the size of the intermolecular contact parameter
. The ordered ß-sheet complex in the folded state and nonaligned ß-sheets or tangled chains in the misfolded state are distinguished by measuring the squared radius of gyration
and the fraction of native contacts Q. The folding yield for the folded state is high at intermediate values of
, but is low at both small and large values of
. The folded state at small
is liquid-like, but is solid-like at both intermediate and large
. The misfolded state at small
contains nonaligned ß-sheets and tangled chains with poor secondary structure at large
. Various folding pathways via dimeric and trimeric intermediates are observed, depending on
. Comparison with experimental results on protein aggregation indicates that intermediate
values are most appropriate for modeling fibril formation and small
values are most appropriate for modeling the formation of amorphous aggregates.
This article has been cited by other articles:
![]() |
B. Ma and R. Nussinov The Stability of Monomeric Intermediates Controls Amyloid Formation: A{beta}25-35 and its N27Q Mutant Biophys. J., May 15, 2006; 90(10): 3365 - 3374. [Abstract] [Full Text] [PDF] |
||||
![]() |
D. Lu, Z. Liu, and J. Wu Structural Transitions of Confined Model Proteins: Molecular Dynamics Simulation and Experimental Validation Biophys. J., May 1, 2006; 90(9): 3224 - 3238. [Abstract] [Full Text] [PDF] |
||||
![]() |
J. K. Cheung and T. M. Truskett Coarse-Grained Strategy for Modeling Protein Stability in Concentrated Solutions Biophys. J., October 1, 2005; 89(4): 2372 - 2384. [Abstract] [Full Text] [PDF] |
||||
![]() |
C. Wu, H. Lei, and Y. Duan The Role of Phe in the Formation of Well-Ordered Oligomers of Amyloidogenic Hexapeptide (NFGAIL) Observed in Molecular Dynamics Simulations with Explicit Solvent Biophys. J., April 1, 2005; 88(4): 2897 - 2906. [Abstract] [Full Text] [PDF] |
||||
![]() |
H. D. Nguyen and C. K. Hall Kinetics of Fibril Formation by Polyalanine Peptides J. Biol. Chem., March 11, 2005; 280(10): 9074 - 9082. [Abstract] [Full Text] [PDF] |
||||
![]() |
H. D. Nguyen and C. K. Hall Phase Diagrams Describing Fibrillization by Polyalanine Peptides Biophys. J., December 1, 2004; 87(6): 4122 - 4134. [Abstract] [Full Text] [PDF] |
||||
![]() |
G. Favrin, A. Irback, and S. Mohanty Oligomerization of Amyloid A{beta}16-22 Peptides Using Hydrogen Bonds and Hydrophobicity Forces Biophys. J., December 1, 2004; 87(6): 3657 - 3664. [Abstract] [Full Text] [PDF] |
||||
![]() |
C. Wu, H. Lei, and Y. Duan Formation of Partially Ordered Oligomers of Amyloidogenic Hexapeptide (NFGAIL) in Aqueous Solution Observed in Molecular Dynamics Simulations Biophys. J., November 1, 2004; 87(5): 3000 - 3009. [Abstract] [Full Text] [PDF] |
||||
| HOME | HELP | FEEDBACK | SUBSCRIPTIONS | ARCHIVE | SEARCH | TABLE OF CONTENTS |