Structure of the Sm binding site from human U4 snRNA derived from a 3 ns PME molecular dynamics simulation

Loss of G-A base pairs is insufficient for achieving a large opening of U4 snRNA K-turn motif

Upon binding to the 15.5K protein, two tandem-sheared G–A base pairs are formed in the internal loop of the kink-turn motif of U4 snRNA (Kt-U4). We have reported that the folding of Kt-U4 is assisted by protein binding. Unstable interactions that contribute to a large opening of the free RNA (‘k–e motion’) were identified using locally enhanced sampling molecular dynamics simulations, results that agree with experiments. A detailed analysis of the simulations reveals that the k–e motion in Kt-U4 is triggered both by loss of G–A base pairs in the internal loop and backbone flexibility in the stems. Essential dynamics show that the loss of G–A base pairs is correlated along the first mode but anti-correlated along the third mode with the k–e motion. Moreover, when enhanced sampling was confined to the internal loop, the RNA adopted an alternative conformation characterized by a sharper kink, opening of G–A base pairs and modified stacking interactions. Thus, loss of G–A base pairs is insufficient for achieving a large opening of the free RNA. These findings, supported by previously published RNA structure probing experiments, suggest that G–A base pair formation occurs upon protein binding, thereby stabilizing a selective orientation of the stems.

Hinge-like motions in RNA kink-turns: the role of the second a-minor motif and nominally unpaired bases

Kink-turn (K-turn) motifs are asymmetric internal loops found at conserved positions in diverse RNAs, with sharp bends in phosphodiester backbones producing V-shaped structures. Explicit-solvent molecular dynamics simulations were carried out for three K-turns from 23S rRNA, i.e., Kt-38 located at the base of the A-site finger, Kt-42 located at the base of the L7/L12 stalk, and Kt-58 located in domain III, and for the K-turn of human U4 snRNA. The simulations reveal hinge-like K-turn motions on the nanosecond timescale. The first conserved A-minor interaction between the K-turn stems is entirely stable in all simulations. The angle between the helical arms of Kt-38 and Kt-42 is regulated by local variations of the second A-minor (type I) interaction between the stems. Its variability ranges from closed geometries to open ones stabilized by insertion of long-residency waters between adenine and cytosine. The simulated A-minor geometries fully agree with x-ray data. Kt-58 and Kt-U4 exhibit similar elbow-like motions caused by conformational change of the adenosine from the nominally unpaired region. Despite the observed substantial dynamics of K-turns, key tertiary interactions are stable and no sign of unfolding is seen. We suggest that some K-turns are flexible elements mediating large-scale ribosomal motions during the protein synthesis cycle.

The snRNP 15.5K protein folds its cognate K-turn RNA: a combined theoretical and biochemical study

The human 15.5K protein binds to the 5' stem-loop of U4 snRNA, promotes the assembly of the spliceosomal U4/U6 snRNP, and is required for the recruitment of the 61K protein and the 20/60/90K protein complex to the U4 snRNA. In the crystallographic structure of the 15.5K-U4 snRNA complex, the conformation of the RNA corresponds to the family of kink-turn (K-turn) structural motifs. We simulated the complex and the free RNA, showing how the protein binding and the intrinsic flexibility contribute to the RNA folding process. We found that the RNA is significantly more flexible in the absence of the 15.5K protein. Conformational transitions such as the interconversion between alternative purine stacking schemes, the loss of G-A base pairs, and the opening of the K-turn occur only in the free RNA. Furthermore, the stability of one canonical G-C base pair is influenced both by the binding of the 15.5K protein and the nature of the adjacent structural element in the RNA. We performed chemical RNA modification experiments and observed that the free RNA lacks secondary structure elements, a result in excellent agreement with the simulations. Based on these observations, we propose a protein-assisted RNA folding mechanism in which the RNA intrinsic flexibility functions as a catalyst.

Molecular dynamics simulations of RNA kissing-loop motifs reveal structural dynamics and formation of cation-binding pockets

Explicit solvent molecular dynamics (MD) simulations were carried out for three RNA kissing-loop complexes. The theoretical structure of two base pairs (2 bp) complex of H3 stem-loop of Moloney murine leukemia virus agrees with the NMR structure with modest violations of few NMR restraints comparable to violations present in the NMR structure. In contrast to the NMR structure, however, MD shows relaxed intermolecular G-C base pairs. The core region of the kissing complex forms a cation-binding pocket with highly negative electrostatic potential. The pocket shows nanosecond-scale breathing motions coupled with oscillations of the whole molecule. Additional simulations were carried out for 6 bp kissing complexes of the DIS HIV-1 subtypes A and B. The simulated structures agree well with the X-ray data. The subtype B forms a novel four-base stack of bulged-out adenines. Both 6 bp kissing complexes have extended cation-binding pockets in their central parts. While the pocket of subtype A interacts with two hexacoordinated Mg2+ ions and one sodium ion, pocket of subtype B is filled with a string of three delocalized Na+ ions with residency times of individual cations 1-2 ns. The 6 bp complexes show breathing motions of the cation-binding pockets and loop major grooves.

Non-Watson-Crick basepairing and hydration in RNA motifs: molecular dynamics of 5S rRNA loop E

Explicit solvent and counterion molecular dynamics simulations have been carried out for a total of >80 ns on the bacterial and spinach chloroplast 5S rRNA Loop E motifs. The Loop E sequences form unique duplex architectures composed of seven consecutive non-Watson-Crick basepairs. The starting structure of spinach chloroplast Loop E was modeled using isostericity principles, and the simulations refined the geometries of the three non-Watson-Crick basepairs that differ from the consensus bacterial sequence. The deep groove of Loop E motifs provides unique sites for cation binding. Binding of Mg(2+) rigidifies Loop E and stabilizes its major groove at an intermediate width. In the absence of Mg(2+), the Loop E motifs show an unprecedented degree of inner-shell binding of monovalent cations that, in contrast to Mg(2+), penetrate into the most negative regions inside the deep groove. The spinach chloroplast Loop E shows a marked tendency to compress its deep groove compared with the bacterial consensus. Structures with a narrow deep groove essentially collapse around a string of Na(+) cations with long coordination times. The Loop E non-Watson-Crick basepairing is complemented by highly specific hydration sites ranging from water bridges to hydration pockets hosting 2 to 3 long-residing waters. The ordered hydration is intimately connected with RNA local conformational variations.

Molecular dynamics simulation of the human U2B" protein complex with U2 snRNA hairpin IV in aqueous solution

A 2200-ps molecular dynamics (MD) simulation of the U2 snRNA hairpin IV/U2B" complex was performed in aqueous solution using the particle mesh Ewald method to consider long-range electrostatic interactions. To investigate the interaction and recognition process between the RNA and protein, the free energy contributions resulting from individual amino acids of the protein component of the RNA/protein complex were calculated using the recently developed glycine-scanning method. The results revealed that the loop region of the U2 snRNA hairpin IV interacted mainly with three regions of the U2B" protein: 1) beta 1-helix A, 2) beta 2-beta 3, and 3) beta 4-helix C. U2 snRNA hairpin IV bound U2B" in a similar orientation as that previously described for U1 snRNA with the U1A' protein; however, the details of the interaction differed in several aspects. In particular, beta 1-helix A and beta 4-helix C in U2B" were not observed to interact with RNA in the U1A' protein complex. Most of the polar and charged residues in the interacting regions had larger mutant free energies than the nonpolar residues, indicating that electrostatic interactions were important for stabilizing the RNA/protein complex. The interaction was further stabilized by a network of hydrogen bonds and salt bridges formed between RNA and protein that was maintained throughout the MD trajectory. In addition to the direct interactions between RNA and the protein, solvent-mediated interactions also contributed significantly to complex stability. A detailed analysis of the ordered water molecules in the hydration of the RNA/protein complex revealed that bridged water molecules reside at the interface of RNA and protein as long as 2100 ps in the 2200-ps trajectory. At least 20 bridged water molecules, on average, contributed to the instantaneous stability of the RNA/protein complex. The stabilizing interaction energy due to bridging water molecules was obtained from ab initio Hartree-Fock and density functional theory calculations.