All-atom Monte Carlo simulation of GCAA RNA folding

被引:20
作者
Nivón, LG
Shakhnovich, EI
机构
[1] Harvard Univ, Dept Chem & Chem Biol, Cambridge, MA 02138 USA
[2] Harvard Univ, Program Biophys, Cambridge, MA 02138 USA
关键词
RNA folding; tetraloop; all-atom Monte Carlo; folding intermediate;
D O I
10.1016/j.jmb.2004.09.041
中图分类号
Q5 [生物化学]; Q7 [分子生物学];
学科分类号
071010 ; 081704 ;
摘要
We report a detailed all-atom simulation of the folding of the GCAA RNA tetraloop. The GCAA tetraloop motif is a very common and thermodynamically stable secondary structure in natural RNAs. We use our simulation methods to study the folding behavior of a 12-base GCAA 2 tetraloop structure with a four-base helix adjacent to the tetraloop proper. We implement an all-atom Monte Carlo (MC) simulation of RNA structural dynamics using a Go potential. Molecular dynamics (MD) simulation of RNA and protein has realistic energetics and sterics, but is extremely expensive in terms of computational time. By coarsely treating noncovalent energetics, but retaining all-atom sterics and entropic effects, all-atom MC techniques are a useful method for the study of protein and now RNA. We observe a sharp folding transition for this structure, and in simulations at room temperature the state histogram shows three distinct minima: an unfolded state (U), a more narrow intermediated state (I), and a narrow folded state (F). The intermediate consists primarily of structures with the GCAA loop and some helix hydrogen bonds formed. Repeated kinetic folding simulations reveal that the number of helix base-pairs forms a simple 1D reaction coordinate for the I --> N transition. (C) 2004 Elsevier Ltd. All rights reserved.
引用
收藏
页码:29 / 45
页数:17
相关论文
共 39 条
[1]   Configurational diffusion down a folding funnel describes the dynamics of DNA hairpins [J].
Ansari, A ;
Kuznetsov, SV ;
Shen, YQ .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 2001, 98 (14) :7771-7776
[2]   A surprising simplicity to protein folding [J].
Baker, D .
NATURE, 2000, 405 (6782) :39-42
[3]   Kinetics of conformational fluctuations in DNA hairpin-loops [J].
Bonnet, G ;
Krichevsky, O ;
Libchaber, A .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 1998, 95 (15) :8602-8606
[4]   Topological and energetic factors: What determines the structural details of the transition state ensemble and "en-route" intermediates for protein folding? An investigation for small globular proteins [J].
Clementi, C ;
Nymeyer, H ;
Onuchic, JN .
JOURNAL OF MOLECULAR BIOLOGY, 2000, 298 (05) :937-953
[5]  
Doi M., 1986, THEORY POLYM DYNAMIC
[6]   On the transition coordinate for protein folding [J].
Du, R ;
Pande, VS ;
Grosberg, AY ;
Tanaka, T ;
Shakhnovich, ES .
JOURNAL OF CHEMICAL PHYSICS, 1998, 108 (01) :334-350
[7]   Monte Carlo update for chain molecules:: Biased Gaussian steps in torsional space [J].
Favrin, G ;
Irbäck, A ;
Sjunnesson, F .
JOURNAL OF CHEMICAL PHYSICS, 2001, 114 (18) :8154-8158
[8]   Protein folding and unfolding at atomic resolution [J].
Fersht, AR ;
Daggett, V .
CELL, 2002, 108 (04) :573-582
[9]   NON-INTERACTING LOCAL-STRUCTURE MODEL OF FOLDING AND UNFOLDING TRANSITION IN GLOBULAR-PROTEINS .1. FORMULATION [J].
GO, N ;
ABE, H .
BIOPOLYMERS, 1981, 20 (05) :991-1011
[10]   Sequence dependent rigidity of single stranded DNA [J].
Goddard, NL ;
Bonnet, G ;
Krichevsky, O ;
Libchaber, A .
PHYSICAL REVIEW LETTERS, 2000, 85 (11) :2400-2403