On the stability of different experimental dimeric structures of the SL1 sequence from the genomic RNA of HIV-1 in solution: A molecular dynamics simulation and electrophoresis study

RNA Structural Dynamics As Captured by Molecular Simulations: A Comprehensive Overview

With both catalytic and genetic functions, ribonucleic acid (RNA) is perhaps the most pluripotent chemical species in molecular biology, and its functions are intimately linked to its structure and dynamics. Computer simulations, and in particular atomistic molecular dynamics (MD), allow structural dynamics of biomolecular systems to be investigated with unprecedented temporal and spatial resolution. We here provide a comprehensive overview of the fast-developing field of MD simulations of RNA molecules. We begin with an in-depth, evaluatory coverage of the most fundamental methodological challenges that set the basis for the future development of the field, in particular, the current developments and inherent physical limitations of the atomistic force fields and the recent advances in a broad spectrum of enhanced sampling methods. We also survey the closely related field of coarse-grained modeling of RNA systems. After dealing with the methodological aspects, we provide an exhaustive overview of the available RNA simulation literature, ranging from studies of the smallest RNA oligonucleotides to investigations of the entire ribosome. Our review encompasses tetranucleotides, tetraloops, a number of small RNA motifs, A-helix RNA, kissing-loop complexes, the TAR RNA element, the decoding center and other important regions of the ribosome, as well as assorted others systems. Extended sections are devoted to RNA-ion interactions, ribozymes, riboswitches, and protein/RNA complexes. Our overview is written for as broad of an audience as possible, aiming to provide a much-needed interdisciplinary bridge between computation and experiment, together with a perspective on the future of the field.

Insight into the intrinsic flexibility of the SL1 stem-loop from genomic RNA of HIV-1 as probed by molecular dynamics simulation

The SL1 stem-loop is the dimerization initiation site for linking the two copies of the RNA forming the HIV-1 genome. The 26 nucleotides stem contains a defect consisting on a highly conserved G-rich 1-3 asymmetrical internal loop, which is a major site for nucleocapsid protein binding. Several NMR attempts were undertaken to determine the internal loop structure in the SL1 monomer. However, the RNA constructs used in the different studies were largely mutated, in particular with replacement of the nine nucleotides apical loop by a tetraloop, and divergent results were obtained ranging from a rigid structure to a particularly large flexibility. To investigate the reasons for such discrepancies, we used molecular dynamics simulation of the SL1 monomer to probe the effect of mutations on the conformational stability of the internal loop and of the whole stem. It is found that in the wild-type sequence, the internal loop displays conformational variability originating mainly from the nine nucleotides apical loop flexibility that causes large conformational fluctuations (without changing the average structure) in the 7 bp duplex linking the apical and internal loops. The large amplitude atomic motions in the duplex are transmitted to the internal loop in which they induce conformational changes characterized by a labile hydrogen bond network such as G5 successively H-bonded to A29 and G30. On the contrary, with a four nucleotides apical loop, conformational fluctuations in the duplex are reduced by a factor of 2 and are not sufficiently energizing for promoting changes in the internal loop structure at the time scale of the simulations.

Conformations of flanking bases in HIV-1 RNA DIS kissing complexes studied by molecular dynamics

Explicit solvent molecular dynamics simulations (in total almost 800 ns including locally enhanced sampling runs) were applied with different ion conditions and with two force fields (AMBER and CHARMM) to characterize typical geometries adopted by the flanking bases in the RNA kissing-loop complexes. We focus on flanking base positions in multiple x-ray and NMR structures of HIV-1 DIS kissing complexes and kissing complex from the large ribosomal subunit of Haloarcula marismortui. An initial x-ray open conformation of bulged-out bases in HIV-1 DIS complexes, affected by crystal packing, tends to convert to a closed conformation formed by consecutive stretch of four stacked purine bases. This is in agreement with those recent crystals where the packing is essentially avoided. We also observed variants of the closed conformation with three stacked bases, while nonnegligible populations of stacked geometries with bulged-in bases were detected, too. The simulation results reconcile differences in positions of the flanking bases observed in x-ray and NMR studies. Our results suggest that bulged-out geometries are somewhat more preferred, which is in accord with recent experiments showing that they may mediate tertiary contacts in biomolecular assemblies or allow binding of aminoglycoside antibiotics.

Molecular dynamics simulation for probing the flexibility of the 35 nucleotide SL1 sequence kissing complex from HIV-1Lai genomic RNA

The SL1 stem-loop located in the encapsidation domain is responsible for initiating the dimerisation of HIV-1 genomic RNA by means of a loop-loop interaction known as Kissing Complex (KC). The SL1 secondary structure has been predicted as a 35 nucleotides [K. G. Murti, M. Bondurant, and A. Tereba. J Virol 37, 411-419 (1981)] stem-loop composed of a 4 base pairs (bp) terminal duplex, a 4 nt asymmetrical internal loop, a 7 bp internal duplex, and a 9 nt apical loop. Several high resolution structures of the monomer and of KC of a 23 nt sequence containing only the internal duplex and the apical loop of SL1 are available in the literature. No experimental high resolution structure of the complete native SL1 sequence has been reported so far, either for the monomer or for KC. The asymmetrical internal loop has been described from NMR studies of different monomeric hairpin sequences, leading to divergent results, which suggests its high flexibility. In this work, we built a SL1(35) KC model which was submitted to a 31 ns molecular dynamics simulation (MD). Our results allows to describe the internal dynamics of SL1(35) KC and the differences of behavior of the different parts of the dimer. Thus, we could show the stability of the interactions between the two apical loops and of the terminal duplexes, the destabilization of the internal duplexes and the high flexibility of the asymmetrical internal loops.

Resolving fast and slow motions in the internal loop containing stem-loop 1 of HIV-1 that are modulated by Mg2+ binding: role in the kissing-duplex structural transition

Stem loop 1 (SL1) is a highly conserved hairpin in the 5'-leader of the human immunodeficiency virus type I that forms a metastable kissing dimer that is converted during viral maturation into a stable duplex with the aid of the nucleocapsid (NC) protein. SL1 contains a highly conserved internal loop that promotes the kissing-duplex transition by a mechanism that remains poorly understood. Using NMR, we characterized internal motions induced by the internal loop in an SL1 monomer that may promote the kissing-duplex transition. This includes micro-to-millisecond secondary structural transitions that cause partial melting of three base-pairs above the internal loop making them key nucleation sites for exchanging strands and nanosecond rigid-body stem motions that can help bring strands into spatial register. We show that while Mg2+ binds to the internal loop and arrests these internal motions, it preserves and/or activates local mobility at internal loop residues G272 and G273 which are implicated in NC binding. By stabilizing SL1 without compromising the accessibility of G272 and G273 for NC binding, Mg2+ may increase the dependence of the kissing-duplex transition on NC binding thus preventing spontaneous transitions from taking place and ensuring that viral RNA and protein maturation occur in concert.

Molecular dynamics simulations of RNA: an in silico single molecule approach

RNA molecules are now known to be involved in the processing of genetic information at all levels, taking on a wide variety of central roles in the cell. Understanding how RNA molecules carry out their biological functions will require an understanding of structure and dynamics at the atomistic level, which can be significantly improved by combining computational simulation with experiment. This review provides a critical survey of the state of molecular dynamics (MD) simulations of RNA, including a discussion of important current limitations of the technique and examples of its successful application. Several types of simulations are discussed in detail, including those of structured RNA molecules and their interactions with the surrounding solvent and ions, catalytic RNAs, and RNA-small molecule and RNA-protein complexes. Increased cooperation between theorists and experimentalists will allow expanded judicious use of MD simulations to complement conceptually related single molecule experiments. Such cooperation will open the door to a fundamental understanding of the structure-function relationships in diverse and complex RNA molecules. .

Polymorphism of bulged-out residues in HIV-1 RNA DIS kissing complex and structure comparison with solution studies

All retroviruses encapsidate their genome as a dimer of homologous single-stranded RNAs. The dimerization initiation site (DIS) of human immunodeficiency virus type 1 (HIV-1) is located in the 5'-untranslated region of the viral genome and consists of a hairpin with a 6 nt self-complementary loop sequence. Genomic RNA dimerization, a crucial step for virion infectivity, is promoted by the formation of a loop-loop complex (or kissing complex) between two DIS hairpins. Crystal structures for the subtypes A, B and F of the HIV-1 DIS kissing complex have now been solved at 2.3 A, 1.9 A and 1.6 A, respectively. They revealed a polymorphism of bulged-out residues showing clearly that their conformation is not a mere consequence of crystal packing. They also provide more insights into ion binding, hydration, and RNA conformation and flexibility. In particular, we observed the binding of spermine to the loop-loop helix, which displaced a magnesium cation important for subtype A DIS dimerization. The excellent agreement between X-ray structures and the results of chemical probing and interference data on larger viral RNA fragments shows that the crystal structures are relevant for the DIS kissing complex present in solution and in viral particles. Accordingly, these structures will be helpful for designing new drugs derived from aminoglycoside antibiotics and targeted against the RNA dimerization step of the viral life-cycle.

Conformational pathway for the kissing complex-->extended dimer transition of the SL1 stem-loop from genomic HIV-1 RNA as monitored by targeted molecular dynamics techniques

HIV-1 retroviral genomic RNA dimerization is initiated by loop-loop interactions between the SL1 stem-loops of two identical RNA molecules. The SL1-SL1 unstable resulting kissing complex (KC) then refolds irreversibly into a more stable complex called extended dimer (ED). Although the structures of both types of complex have been determined, very little is known about the conformational pathway corresponding to the transition, owing to the difficulty of observing experimentally intermediate conformations. In this study, we applied targeted molecular dynamics simulation techniques (TMD) to the phosphorus atoms for monitoring this pathway for the backbone, and a two-step strategy was adopted. In a first step, called TMD(-1), the dimer structure was constrained to progressively move away from KC without indicating the direction, until the RMSD from KC reaches 36A. A total of 20 TMD(-1) simulations were performed under different initial conditions and different simulation parameters. For RMSD ranging between 0 and 22A, the whole set of TMD(-1) simulations follows a similar pathway, then divergences are observed. None of the simulations leads to the ED structure. At RMSD=22A, the dimers look like two parallel Us, still linked by the initial loop-loop interaction, but the strands of the stems (the arms of the Us) are positioned in such a manner that they can form intramolecular as well as intermolecular Watson-Crick base-pairs. This family of structure is called UU. In a second step (TMD simulations), 18 structures were picked up along the pathways generated with TMD(-1) and were constrained to move toward ED by decreasing progressively their RMSD from ED. We found that only structures from the UU family are able to easily reach ED-like conformations of the backbones without exhibiting a large constraint energy.

Dynamics and Stability of GCAA Tetraloops with 2-Aminopurine and Purine Substitutions

The contributions of various interactions in the GGCGCAAGCC hairpin containing a GCAA tetraloop were studied by computer simulations using the substitutions of functional groups. The guanosine (G) in the first tetraloop position or in the C-G closing base pair was replaced by 2-aminopurine (AP), and the individual tetraloop's adenosines (A) were replaced by purine (PUR). These substitutions eliminated particular hydrogen bonds thought to stabilize the GCAA tetraloop. For each substitution, molecular dynamics (MD) simulations were carried out in an aqueous solution with sodium counterions, using the CHARMM27 force field. The MD simulations showed that the substitutions in the first (G-->AP) and the third (A-->PUR) position of the GCAA tetraloop did not significantly influence the conformation of the hairpin. A long-lived bridging water molecule observed in the GCAA loop was present in both modified loops. The substitutions made in the last loop position (A-->PUR) or in the C-G base pair closing the tetraloop (G-->AP) to some extent influenced the loop structure and dynamics. These loops did not display the long-lived bridging water molecules. When the second A in the GCAA loop was replaced by PUR, the first A in the loop was observed in the anti or in the syn orientation about the glycosyl bond. The G to AP substitution in C-G base pair led to a change of their arrangement from the Watson-Crick to wobble. The MD simulations of the hairpin with C-AP wobble closing base pair showed increased conformational dynamics of the hairpin. The changes of hairpin formation free energy associated with the substitutions of individual bases were calculated by the free energy perturbation method. Our theoretical estimates suggest a larger destabilization for the G to AP substitutions in GCAA loop than for the substitutions of individual A's by PUR, which is in accordance with experimental tendency. The calculations predicted a similar free energy change for G to AP substitutions in the GCAA tetraloop and in the C-G closing base pair.