Effects of osmolytes on stable UUCG tetraloops and their preference for a CG closing base pair

Osmolytes have the potential to affect the stability of secondary structure motifs and alter preferences for conserved nucleic acid sequences in the cell. To contribute to the understanding of the in vivo function of RNA we observed the effects of different classes of osmolytes on the UNCG tetraloop motif. UNCG tetraloops are the most common and stable of the RNA tetraloops and are nucleation sites for RNA folding. They also have a significant thermodynamic preference for a CG closing base pair. The thermal denaturation of model hairpins containing UUCG loops was monitored using UV-Vis spectroscopy in the presence of osmolytes with different chemical properties. Interestingly, all of the osmolytes tested destabilized the hairpins, but all had little effect on the thermodynamic preference for a CG base pair, except for polyethylene glycol (PEG) 200. PEG 200 destabilized the loop with the CG closing base pair relative to the loop with a GC closing base pair. The destabilization was linear with increasing concentrations of PEG 200, and the slope of this relationship was not perturbed by changes in the hairpin stem outside of the closing pair. This result suggests that in the presence of PEG 200, the UUCG loop with a GC closing base pair may retain some preferential interactions with the cosolute that are lost in the presence of the CG closing base pair. These results reveal that relatively small structural changes may influence how osmolytes tune the stability, and thus the function of a secondary structure motif in vivo.     

Enhanced loop DNA folding induced by thymine-CH3 group contact and perpendicular guanine-thymine interaction

A remarkable stabilizing effect induced by T-CH₃ group and perpendicular guanine–thymine interactions in the DNA loop conformation has been demonstrated for the d(TTTG) loop structure using UV melting, high resolution NMR, distance geometry, and molecular dynamics studies. Contrary to the previously published d(TTCG) sequence that exhibits no specific inter-nucleotide interaction, we have found that d(TTTG), which differs only by one nucleotide with the d(TTCG) sequence (C7 T7), forms a rather stable and well-defined loop structure. Two characteristic structural features account for the stabilization of an otherwise flexible loop structure; the second loop T (T6) residue folds into the minor groove and engages in perpendicular interaction with the G8-NH₂, while the third loop T (T7) residue stacks well upon the closing T5G8 wobble base pair and exhibits good contacts with many of the loop T5 and T6 sugar protons, which may form a hydrophobic core in the loop region. The importance of the bulky T7-CH₃ was also proved by the UV melting study; while d(TTCG) hairpin exhibits a lower melting point (74.5°C ) than d(TTTG) hairpin (80.5°C ), d(TT^5–methylCG) hairpin resumes the same higher melting point (80°C ). Similarly, the fact that the melting temperature (74°C ) of d(TTTI) is lower than that of d(TTTG) indicates the critical role played by the G8-NH₂ group. Our structural studies of the d(TTTG) loop indicate that DNA and RNA use a different strategy to establish stable tertiary folds. Comparison with several other pyrimidine-rich loop hairpins suggests that different minor-groove folding modes exist for the folding thymidine residue.     

A molecular dynamics simulation of the flavin mononucleotide–RNA aptamer complex

We report on an unrestrained molecular dynamics simulation of the flavin mononucleotide (FMN)–RNA aptamer. The simulated average structure maintains both cross‐strand and intermolecular FMN–RNA nuclear Overhauser effects from the nmr experiments and has all qualitative features of the nmr structure including the G10–U12–A25 base triple and the A13–G24, A8–G28, and G9–G27 mismatches. However, the relative orientation of the hairpin loop to the remaining part of the molecule differs from the nmr structure. The simulation predicts that the flexible phosphoglycerol part of FMN moves toward G27 and forms hydrogen bonds. There are structurally long‐lived water molecules in the FMN binding pocket forming hydrogen bonds within FMN and between FMN and RNA. In addition, long‐lived water is found bridging primarily RNA backbone atoms. A general feature of the environment of long‐lived “structural” water is at least two and in most cases three or four potential acceptor atoms. The 2′‐OH group of RNA usually acts as an acceptor in interactions with the solvent. There are almost no intrastrand O2′H(n)⋮O4′(n + 1) hydrogen bonds within the RNA backbone. In the standard case the preferred orientation of the 2′‐OH hydrogen atoms is approximately toward O3′ of the same nucleotide. However, a relatively large number of conformations with the backbone torsional angle γ in the trans orientation is found. A survey of all experimental RNA x‐ray structures shows that this backbone conformation occurs but is less frequent than found in the simulation. Experimental nmr RNA aptamer structures have a higher fraction of this conformation as compared to the x‐ray structures. The backbone conformation of nucleotide n + 1 with the torsional angle γ in the trans orientation leads to a relatively short distance between 2′‐OH(n) and O5′(n + 1), enabling hydrogen‐bond formation. In this case the preferred orientation of the 2′‐OH hydrogen atom is approximately toward O5′(n + 1). We find two relatively short and dynamically stable types of backbone–backbone next‐neighbor contacts, namely C2′(H)(n)⋮O4′(n + 1) and C5′(H)(n + 1)⋮O2′(n). These interactions may affect both backbone rigidity and thermodynamic stability of RNA helical structures. © 1999 John Wiley & Sons, Inc. Biopoly 50: 287–302, 1999