A-Site Residues Move Independently from P-Site Residues in all-Atom Molecular Dynamics Simulations of the 70S Bacterial Ribosome
Pande VS (2012) A-Site Residues Move Independently from P-Site Residues in all-Atom Molecular Dynamics Simulations of
the 70S Bacterial Ribosome. PLoS ONE 7(1): e29377. doi:10.1371/journal.pone.0029377
A-Site Residues Move Independently from P-Site Residues in all-Atom Molecular Dynamics Simulations of the 70S Bacterial Ribosome
Relly Brandman 0
Yigal Brandman 0
Vijay S. Pande 0
Jie Zheng, University of Akron, United States of America
0 1 Chemical and Systems Biology, Stanford University, Stanford, California, United States of America, 2 Chemistry, Stanford University , Stanford, California , United States of America
The ribosome is a large macromolecular machine, and correlated motion between residues is necessary for coordinating function across multiple protein and RNA chains. We ran two all-atom, explicit solvent molecular dynamics simulations of the bacterial ribosome and calculated correlated motion between residue pairs by using mutual information. Because of the short timescales of our simulation (ns), we expect that dynamics are largely local fluctuations around the crystal structure. We hypothesize that residues that show coupled dynamics are functionally related, even on longer timescales. We validate our model by showing that crystallographic B-factors correlate well with the entropy calculated as part of our mutual information calculations. We reveal that A-site residues move relatively independently from P-site residues, effectively insulating A-site functions from P-site functions during translation.
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Funding: RB was funded by a Bio-X Graduate Student Fellowship. Computer resources on the Stanford Bio-X2 cluster were provided by National Science
Foundation award Division of Computer and Network Systems CNS-0619926. The funders had no role in study design, data collection and analysis, decision to
publish, or preparation of the manuscript.
Competing Interests: The authors have declared that no competing interests exist.
The dynamic motion of macromolecular machines such as the
ribosome is coordinated across multiple chains to accomplish
complex, multi-step functions and elucidation of these motions is
fundamental to understanding how these large machines work
[1,2,3,4,5]. The ribosome translates mRNA into protein by
coordinated dynamics of its hundreds of thousands of atoms in
more than fifty RNA and protein chains. These chains are
assembled into two subunits: the large subunit catalyzes peptide
bond formation, and the small subunit decodes mRNA by
facilitating the binding of the mRNA codon to the corresponding
tRNA anticodon. Co-factors and GTP hydrolysis catalyze events
in protein synthesis, however the ability of the ribosome to
translate without GTP hydrolysis [6] and even without any
cofactors [7,8] suggests that functionally important dynamics are
intrinsic to the ribosome itself. The molecular details of ribosomal
translation are still an active area of research, and understanding
ribosome dynamics is central to understanding how this robust
molecular machine orchestrates protein synthesis.
Our current understanding of ribosome dynamics began largely
by comparing EM and x-ray crystallography structures of the
ribosome in various states (for example bound to co-factors or
tRNA) [1,2,3,4]. The ribosome translates proteins on the order of
seconds (e.g. ,20 amino acids per second in Escherichia coli).
Largescale dynamics such as motion in the GTPase association center
[9] and L1 stalk [10] (large subunit protuberances at the tRNA
entrance and exit sites, respectively) have been measured on
similar timescales using methods such as single molecule
fluorescence resonance energy transfer (smFRET) [10,11,12].
Thus enzymatic timescales are on the seconds timescales, and
there is likely a broad range of timescales characterizing ribosome
dynamics. Elucidating motions in the ribosome continues to be an
active area of research by both experimental and computational
methods.
Computational models of ribosome dynamics are challenging
because of the ribosomes large size. Methods for modeling
enzyme dynamics range from reduced complexity coarse-grained
models to the all-atom detail of explicit solvent molecular
dynamics simulations (MD) [13,14,15,16,17]. The more detail
included in a computational model, the more computationally
demanding the calculations are. Coarse-grained models are able to
access biologically relevant timescales (e.g. peptide bond formation
occurs on the seconds timescale), while more detailed models such
as MD require decades of CPU years to reach tens of nanoseconds
for the millions of atoms in a system as large as the ribosome.
Multiple, independent models of ribosome dynamics on various
timescales complement each other and fill in molecular-level
spatial and temporal timescales that can be difficult to access
experimentally.
Our goal is to find features in nanosecond length all-atom MD
of ribosome dynamics that are biologically relevant. Correlated
motions have been previously linked to enzyme function [18],
including coarse-grained simulations of the ribosome on the
seconds timescale [15]. Correlated motions in short timescale
(relative to biological timescales) MD have been used to gain
insight in other systems (e.g. [19]). We expect that the ns dynamics
in our simulations are largely from thermal motions and local
conformational changes around the crystal structure rather than
large-scale conformational changes. We calculate correlated
motion in order to group atoms with coupled dynamics together.
We hypothesize that atoms with coupled dynamics are functionally
related, and that these relationships are also relevant on longer
timescales.
Here we present data from two all-atom MD trajectories of the
complete (both subunits, 70S) bacterial Thermus Thermophilus
bacterial ribosome [20] and calculate correlations in residue
dynamics using mutual information. One trajectory is of the
ribosome alone (53 ns), and the other trajectory contains the
ribosome with mRNA and tRNA (32 ns). Because of the short
timescale (compared to the timescale for translation) and the fact
that the initial starting configuration reflects a stalled ribosome in
the pre-translocation state, we do not expect to see motions
corresponding to translation. We expect that motions in our
simulation are largely thermal motions on the ns timescale and
local conformational changes around the crystal structure, thus
our conclusions can be likened to characterizing a structure based
on how it vibrates. We describe correlated motions between
residues in order to characterize groups of atoms that may
function together as parts of the larger macromolecular
machine, thus providing insight into ribosome dynamics.
Correlated motions corroborate previously established parts such as
the two symmetry-related regions in the active site [21] and the
peptide exit tunnel constriction site formed by two proteins [22].
Residues in the large subunit along the path of tRNA
transloc (...truncated)