Conformational transitions using molecular dynamics with minimum biasing

The molecular dynamics algorithm (MD), which simulates intramolecular motions on the subnanosecond timescale, has been modified to allow the investigation of slow conformational transitions that do not necessarily occur spontaneously in MD simulations. The method is designated CONTRA MD (CONformational TRAnsitions by Molecular Dynamics with minimum biasing). The method requires the prior definition of a single conformational variable that is required to vary monotonically from an initial conformation to a final target conformation. The simulation is broken up into a series of short free MD segments, and we determine, after each segment of MD, whether or not the system has evolved toward the final conformation. Those segments that do not move the system in that direction are deleted. Those that do move it toward the final conformation are patched together sequentially to generate a single representative trajectory along the transition pathway. The CONTRA MD method is demonstrated first by application to the simultaneous C2′‐endo to C3′‐endo repucker and anti to syn N‐glycosidic torsion transitions in 2′‐deoxyadenosine and then to the large‐scale bending in phenylalanine transfer RNA. © 1993 John Wiley & Sons, Inc.

[1]  C. Tung A reduced set of coordinates for modeling DNA structures: (I). A B-to-A transition pathway driven by pseudorotational angle. , 1992, Journal of biomolecular structure & dynamics.

[2]  R. Elber,et al.  Reaction path study of conformational transitions in flexible systems: Applications to peptides , 1990 .

[3]  Wilma K. Olson How flexible is the furanose ring? 2. An updated potential energy estimate , 1982 .

[4]  M. Karplus,et al.  The hinge-bending mode in lysozyme , 1976, Nature.

[5]  J. Mccammon,et al.  Molecular‐dynamics simulation of phenylalanine transfer RNA. I. Methods and general results , 1985, Biopolymers.

[6]  J A McCammon,et al.  Phenylalanine transfer RNA: molecular dynamics simulation. , 1984, Science.

[7]  Wolfram Saenger,et al.  Principles of Nucleic Acid Structure , 1983 .

[8]  Ron Elber,et al.  A new technique to calculate steepest descent paths in flexible polyatomic systems , 1990 .

[9]  J. Mccammon,et al.  Intramolecular flexibility in phenylalanine transfer RNA , 1981, Nature.

[10]  Stephen C. Harvey,et al.  Ribose puckering: structure, dynamics, energetics, and the pseudorotation cycle , 1986 .

[11]  P. Kollman,et al.  An all atom force field for simulations of proteins and nucleic acids , 1986, Journal of computational chemistry.

[12]  J A McCammon,et al.  Large‐amplitude bending motions in phenylalanine transfer RNA , 1984, Biopolymers.

[13]  Charles L. Brooks,et al.  Molecular dynamics with internal coordinate constraints , 1988 .

[14]  J. Mccammon,et al.  Dynamics of Proteins and Nucleic Acids , 2018 .

[15]  Arieh Warshel,et al.  Extreme conformational flexibility of the furanose ring in DNA and RNA , 1978 .

[16]  B. Hingerty,et al.  Further refinement of the structure of yeast tRNAPhe. , 1978, Journal of molecular biology.