Unusual nucleotide conformations in GNRA and UNCG type tetraloop hairpins: evidence from Raman markers assignments.

High resolution NMR data on UNCG and GNRA tetraloops (where N is any of the four nucleotides and R is a purine) have shown that they contain ribonucleosides with unusual 2'-endo/anti and 3'-endo/syn conformations, in addition to the 3'-endo/anti ones which are regularly encountered in RNA chains. In the current study, Raman spectroscopy has been used to probe these nucleoside conformations and follow the order (hairpin) to disorder (random chain) structural transitions in aqueous phase in the 5-80 degreesC temperature range. Spectral evolution of GCAA and GAAA tetraloops, as formed in very short hairpins with only three G.C base pairs in their stems (T m >60 degreesC), are reported and compared with those previously published on UUCG and UACG tetraloops, for which the syn orientation of the terminal guanine as well as the 2'-endo/anti conformation of the third rC residue have been confirmed by means of vibrational marker bands. Raman data obtained as a function of temperature show that the first uracil in the UUCG tetraloop is stacked and the two middle residues (rU and rC) are in the 2'-endo/anti conformation, in agreement with the previously published NMR results. As far as the new data concerning the GNRA type tetraloops are concerned, they lead us to conclude that: (i) in both cases (GCAA and GAAA tetraloops) the adenine bases are stacked; (ii) the second rC residue in the GCAA tetraloop has a 3'-endo/anti conformation; (iii) the sugar pucker associated with the third rA residue in both tetraloops possibly undergoes a 3'-endo/2'-endo interconversion as predicted by NMR results; (iv) the stem adopts a regular A-form structure; (v) all other nucleosides of these two GNRA tetraloops possess the usual 3'-endo/anti conformation.     

Important role of the tetraloop region of 4.5S RNA in SRP binding to its receptor FtsY

Binding of Escherichia coli signal recognition particle (SRP) to its receptor, FtsY, requires the presence of 4.5S RNA, although FtsY alone does not interact with 4.5S RNA. In this study, we report that the exchange of the GGAA tetraloop sequence in domain IV of 4.5S RNA for UUCG abolishes SRP-FtsY interaction, as determined by gel retardation and membrane targeting experiments, whereas replacements with other GNRA-type tetraloops have no effect. A number of other base exchanges in the tetraloop sequence have minor or intermediate inhibitory effects. Base pair disruptions in the stem adjacent to the tetraloop or replacement of the closing C-G base pair with G-C partially restored function of the otherwise inactive UUCG mutant. Chemical probing by hydroxyl radical cleavage of 4.5S RNA variants show that replacing GGAA with UUCG in the tetraloop sequence leads to structural changes both within the tetraloop and in the adjacent stem; the latter change is reversed upon reverting the C-G closing base pair to G-C. These results show that the SRP-FtsY interaction is strongly influenced by the structure of the tetraloop region of SRP RNA, in particular the tetraloop stem, and suggest that both SRP RNA and Ffh undergo mutual structural adaptation to form SRP that is functional in the interaction with the receptor, FtsY.     

Comparison between CUUG and UUCG tetraloops: thermodynamic stability and structural features analyzed by UV absorption and vibrational spectroscopy

CUUG loop is one of the most frequently occurring tetraloops in bacterial 16S rRNA. This tetraloop has a high thermodynamic stability as proved by previous UV absorption and NMR experiments. Here, we present our results concerning the thermodynamic and structural features of the 10mer 5′-r(GCG-CUUG-CGC)-3′, forming a highly stable CUUG tetraloop hairpin in aqueous solution, by means of several optical techniques (UV and FT-IR absorption, Raman scattering). UV melting profile of this decamer provides a high melting temperature (60.7°C). A set of Raman spectra recorded at different temperatures allowed us to analyze the order-to-disorder (hairpin-to-random coil) transition. Assignment of vibrational markers led us to confirm the particular nucleoside conformation, and to get information on the base stacking and base pairing in the hairpin structure. Moreover, comparison of the data obtained from two highly stable CUUG and UUCG tetraloops containing the same nucleotides but in a different order permitted an overall discussion of their structural features on the basis of Raman marker evidences.     

Rearrangement of partially ordered stacked conformations contributes to the rugged energy landscape of a small RNA hairpin

We have studied the fast relaxation kinetics of a small RNA hairpin tetraloop using time-resolved infrared spectroscopy. A laser-induced temperature jump initiated the relaxation by rapidly perturbing the thermal equilibrium of the sample. We probed the relaxation kinetics at two different wavenumbers, 1574 and 1669 cm (-1). The latter is due to the C6O6 carbonyl stretch of the base guanine and is a direct measure of guanine base pairing. The former is assigned to a ring vibration of guanine and tracks structure by sensing base stacking interactions. Overall, the kinetics at 1574 cm (-1) are faster than those observed at 1669 cm (-1). When relaxation occurs at the melting temperature, the kinetics at both wavenumbers are biexponential. When relaxation occurs at a temperature that is higher than the melting temperature, the data at 1669 cm (-1) are still biexponential while only a single fast phase is resolved in the data at 1574 cm (-1). The fast phases are in the range of microseconds, while the slower phases are in the range of tens of microseconds. At both wavenumbers, a portion of the relaxation is not resolved, indicating the existence of a very fast, sub-100 ns phase. Our results provide additional evidence that small, fast folding hairpin loops are characterized by a rugged energy landscape. Furthermore, our data suggest that single-strand stacking interactions and stacking interactions in the loop contribute significantly to the ruggedness of the energy landscape. This work also demonstrates the utility of time-resolved infrared spectroscopy in studying RNA folding.     

Stem-loop structures can effectively substitute for an RNA pseudoknot in -1 ribosomal frameshifting

-1 Programmed ribosomal frameshifting (PRF) in synthesizing the gag-pro precursor polyprotein of Simian retrovirus type-1 (SRV-1) is stimulated by a classical H-type pseudoknot which forms an extended triple helix involving base-base and base-sugar interactions between loop and stem nucleotides. Recently, we showed that mutation of bases involved in triple helix formation affected frameshifting, again emphasizing the role of the triple helix in -1 PRF. Here, we investigated the efficiency of hairpins of similar base pair composition as the SRV-1 gag-pro pseudoknot. Although not capable of triple helix formation they proved worthy stimulators of frameshifting. Subsequent investigation of ～30 different hairpin constructs revealed that next to thermodynamic stability, loop size and composition and stem irregularities can influence frameshifting. Interestingly, hairpins carrying the stable GAAA tetraloop were significantly less shifty than other hairpins, including those with a UUCG motif. The data are discussed in relation to natural shifty hairpins.     

Thermodynamics of 2'-ribose substitutions in UUCG tetraloops

The ribose 2'-hydroxyl group confers upon RNA many unique molecular properties. To better appreciate its contribution to structure and stability and to monitor how substitutions of the 2' hydroxyl can alter an RNA molecule, each loop pyrimidine ribonucleotide in the UUCG tetraloop was substituted with a nucleotide containing either a fluorine (2'-F), hydrogen (2'-H), amino (2'-NH2), or methoxy (2'-OCH3) group, in the context of both the C:G and G:C loop-closing base pair. The thermodynamic parameters of these tetraloop variants have been determined and NMR experiments used to monitor the structural changes resulting from the substitutions. The modified riboses are better tolerated in the G[UUCG]C tetraloop, which may be due to its increased loop flexibility relative to the C[UUCG]G loop. Even for these simple substitutions, the free-energy change reflects a complex interplay of hydrogen bonding, solvation effects, and intrinsic pucker preferences of the nucleotides.     

The crystal structure of UUCG tetraloop

All large structured RNAs contain hairpin motifs made of a stem closed by several looped nucleotides. The most frequent loop motif is the UUCG one. This motif belongs to the tetraloop family and has the peculiarity of being highly thermodynamically stable. Here, we report the first crystal structure of two UUCG tetraloops embedded in a larger RNA-protein complex solved at 2.8 A resolution. The two loops present in the asymmetric unit are in a different crystal packing environment but, nevertheless, have an identical conformation. The observed structure is globally close to that obtained in solution by nuclear magnetic resonance. However, subtle differences point to a more detailed picture of the role played by 2'-hydroxyl groups in stabilising this tetraloop.     

NMR structure of the 3' stem-loop from human U4 snRNA

The NMR structure of the 3' stem-loop (3'SL) from human U4 snRNA was determined to gain insight into the structural basis for conservation of this stem-loop sequence from vertebrates. 3'SL sequences from human, rat, mouse and chicken U4 snRNA each consist of a 7 bp stem capped by a UACG tetraloop. No high resolution structure has previously been reported for a UACG tetraloop. The UACG tetraloop portion of the 3'SL was especially well defined by the NMR data, with a total of 92 NOE-derived restraints (about 15 per residue), including 48 inter-residue restraints (about 8 per residue) for the tetraloop and closing C-G base pair. Distance restraints were derived from NOESY spectra using MARDIGRAS with random error analysis. Refinement of the 20mer RNA hairpin structure was carried out using the programs DYANA and miniCarlo. In the UACG tetraloop, U and G formed a base pair stabilized by two hydrogen bonds, one between the 2'-hydroxyl proton of U and carbonyl oxygen of G, another between the imino proton of G and carbonyl oxygen O2 of U. In addition, the amino group of C formed a hydrogen bond with the phosphate oxygen of A. G adopted a syn orientation about the glycosidic bond, while the sugar puckers of A and C were either C2'-endo or flexible. The conformation of the UACG tetraloop was, overall, similar to that previously reported for UUCG tetraloops, another member of the UNCG class of tetraloops. The presence of an A, rather than a U, at the variable position, however, presents a distinct surface for interaction of the 3'SL tetraloop with either RNA or protein residues that may stabilize interactions important for active spliceosome formation. Such tertiary interactions may explain the conservation of the UACG tetraloop motif in 3'SL sequences from U4 snRNA in vertebrates.     

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.     

Common Structural Features of UUCG and UACG Tetraloops in Very Short Hairpins Determined by UV Absorption,Raman, IR and NMR Spectroscopies

Abstract

Thermodynamic and structural properties of two UNCG tetraloops in very short hairpin octamers, 5′-r (GCUUCGGC)-3′ and 5′-r (GCUACGGC)-3′. have been studied by means of various physical techniques. Melting profiles of both octamers, obtained from UV absorption spectra taken as a function of temperature, are consistent with a monophasic, progressive and completely reversible order-to-disorder transition and confirm their unusual structural stability (T_m>51^° C). The ¹H, ¹³C and ³¹P NMR chemical shifts and coupling constants of the UACG loop nucleotides are comparable with those reported previously for UUCG loops, i.e. 2′-endo/anti conformation of the second and third nucleotide of the loop as well as the syn orientation of the ultimate guanine base and the A-type double helical conformation of the hairpin stem. Simulation of quantitative NOESY volumes shows that the UACG octamer adopts a very rigid compact structure which is well represented by an average order parameter of 0.9. Three base-pairs and four additional strong hydrogen bonds are undoubtedly responsible for such limited flexibility. Raman and infrared spectra as a function of temperature reflect the order-to-disorder transition, as well. Vibrational conformational markers in low temperature spectra of both octamers indicate the hairpin structure as the major conformer in aqueous phase. These spectra further support the structural features of most of the nucleotides involved in the tetraloops and clearly demonstrate the structural similarities of the phosphodiester backbone in both hairpins. Consequently, on the basis of all present results, one can deduce that the conformational features of the UUCG and UACG tetraloops seem to be inherent to the UNCG type tetraloops, regardless of either the nature of the tetraloop second base or the stem length.     

Effects of base substitutions in an RNA hairpin from molecular dynamics and free energy simulations

Contributions of individual interactions in the GGCGCAAGCC hairpin containing a GCAA tetraloop were studied by computer simulations using base substitutions. The G in the first tetraloop position was replaced by inosine (I) or adenosine (A), and the G in the C-G basepair closing the tetraloop was replaced by I. These substitutions eliminate particular hydrogen bonds proposed in the nuclear magnetic resonance model of the GCAA tetraloop. Molecular dynamics simulations of the GCAA tetraloop in aqueous solvent displayed a well-defined hydrogen pattern between the first and last loop nucleotides (G and A) stabilized by a bridging water molecule. Substitution of G-->I in the basepair closing the tetraloop did not significantly influence the loop structure and dynamics. The ICAA loop maintained the overall structure, but displayed variation in the hydrogen-bond network within the tetraloop itself. Molecular dynamics simulations of the ACAA loop led to conformational heterogeneity of the resulting structures. Changes of hairpin formation free energy associated with substitutions of individual bases were calculated by the free energy perturbation method. The calculated decrease of the hairpin stability upon G-->I substitution in the C-G basepair closing the tetraloop was in good agreement with experimental thermodynamic data. Our theoretical estimates for G-->I and G-->A mutations located in the tetraloop suggest larger loop destabilization than corresponding experimental results. The extent of conformational sampling of the structures resulting from base substitutions and its impact on the calculated free energy was discussed.     

Molecular modelling of the 3-D structure of RNA tetraloops with different nucleotide sequences.

One surprisingly common element of RNA secondary structure consists of a hairpin capped by a four-base loop (or the tetraloop). Recently the 3-D structures of two RNA-tetraloops have been determined by NMR-studies. Both structures have a similar architecture: the first and the last bases of the loop form a hydrogen bonded pair which is stacked on the stem base pair. We have analysed the ability of tetraloops, with the other combinations of the first and the fourth bases, to adopt such a 'diloop' conformation using computer modelling. The analysis has shown that the 'diloop' conformation has many covalent and steric constraints which give a possibility for reliable structural predictions. As a result, a set of the tetraloop 3-D structures in which hydrogen bonded pairing of the first and the last bases does not cause covalent and steric hindrances has been selected. In most cases several predicted 3-D structures corresponded to one tetraloop sequence. Taking into consideration the folding pathway of RNA hairpins we have resolved this ambiguity and predicted the most probable 3-D structure for every possible nucleotide sequence of the tetraloop. On the basis of these results a conclusion has been drawn on the possible reasons of the tetraloop phylogenetic preference.     

Thermal stability, structural features, and B-to-Z transition in DNA tetraloop hairpins as determined by optical spectroscopy in d(CG)(3)T(4)(CG)(3) and d(CG)(3)A(4)(CG)(3) oligodeoxynucleotides

NMR and CD data have previously shown the formation of the T(4) tetraloop hairpin in aqueous solutions, as well as the possibility of the B-to-Z transition in its stem in high salt concentration conditions. It has been shown that the stem B-to-Z transition in T(4) hairpins leads to S (south)- to N (north)-type conformational changes in the loop sugars, as well as anti to syn orientations in the loop bases. In this article, we have compared by means of UV absorption, CD, Raman, and Fourier transform infrared (FTIR), the thermodynamic and structural properties of the T(4) and A(4) tetraloop hairpins formed in 5'-d(CGCGCG-TTTT-CGCGCG)-3' and 5'-d(CGCGCG-AAAA-CGCGCG)-3', respectively. In presence of 5M NaClO(4), a complete B-to-Z transition of the stems is first proved by CD spectra. UV melting profiles are consistent with a higher thermal stability of the T(4) hairpin compared to the A(4) hairpin. Order-to-disorder transition of both hairpins has also been analyzed by means of Raman spectra recorded as a function of temperature. A clear Z-to-B transition of the stem has been confirmed in the T(4) hairpin, and not in the A(4) hairpin. With a right-handed stem, Raman and FTIR spectra have confirmed the C2'-endo/anti conformation for all the T(4) loop nucleosides. With a left-handed stem, a part of the T(4) loop sugars adopt a N-type (C3'-endo) conformation, and the C3'-endo/syn conformation seems to be the preferred one for the dA residues involved in the A(4) tetraloop.     

Structure of 2',5'-linked tetraribonucleotide loops: a novel RNA motif

We report on the three dimensional structure of an RNA hairpin containing a 2',5'-linked tetraribonucleotide loop, namely, 5'-rGGAC(UUCG)GUCC-3' (where UUCG = U(2'p5')U(2'p5')C(2'p5')G(2'p5')). We show that the 2',5'-linked RNA loop adopts a conformation that is quite different from that previously observed for the native 3',5'-linked RNA loop. The 2',5'-RNA loop is stabilized by (a) U:G wobble base pairing, with both bases in the anti conformation, (b) extensive base stacking, and (c) sugar-base contacts, all of which contribute to the extra stability of this hairpin structure.     

Solution structure of Cobalt(III)hexammine complexed to the GAAA tetraloop, and metal-ion binding to G.A mismatches

The solution structure of a 22 nt RNA hairpin and its complex with Co(NH(3))(6)(3+) bound to the GAAA tetraloop has been determined by NMR spectroscopy. Co(NH(3))(6)(3+) has a similar geometry to Mg(H(2)O)(6)(2+) and can be used as a probe for binding sites of completely solvated magnesium ions. The hairpin contains tandem G.A mismatches, similar to the P5abc region of a group I intron, and is closed by a GAAA tetraloop. The tandem G.A mismatches are imino hydrogen bonded in contrast with the sheared G.A mismatches found in a different context in the crystal structure of the P4-P6 domain. Chemical shift changes of the imino protons upon titration of the RNA hairpin with Mg(2+) and with Co(NH(3))(6)(3+) were used to identify ion-binding sites. Paramagnetic resonance broadening upon titration with Mn(2+) was also used. The titration curves gave dissociation binding constants for the magnesium ions in the millimolar range, similar to the binding in the major groove of RNA at tandem G.U base-pairs. Although the largest chemical shift change occurred at an imino proton of one of the G.A base-pairs, no nuclear Overhauser enhancement cross-peaks between the cobalt ligand and neighboring RNA protons were seen, presumably due to the high mobility of the Co(NH(3))(6)(3+) at this site. Nuclear Overhauser enhancement cross-peaks between Co(NH(3))(6)(3+) and the GAAA tetraloop were observed, which allowed the determination of the structure of the tetraloop binding site. The Co(NH(3))(6)(3+) is bound in the major groove of the GAAA tetraloop with hydrogen bonds to guanine base N7 and to phosphate oxygen atoms of the tetraloop.     

Preference for ribose over deoxyribose in loop-closing base pairs of extra stable nucleic acid hairpins

We have investigated the effect of switching ribose to deoxyribose at the closing base-pair of an extra-stable RNA hairpin. Specifically, we studied the sequence 5'-GGAC(UUCG)GUCC, a dodecanucleotide that folds into a well-characterized, "extra stable" RNA hairpin structure. Recently, we showed that hairpins containing a 2',5'-linked (UUCG) loop instead of the native 3',5'-linked loop also exhibit extra-stability (Hannoush and Damha, J. Am. Chem. Soc., 2001, 123, 12368-12374). In this article, we show that the ribose units located at the loop-closing positions (i.e., rC4 and rG9) contribute significantly to the stabilization of RNA hairpins, particularly those containing the 3',5'-UUCG loop. Interestingly, the requirement of rC4 and rG9 is more relaxed for DNA hairpins containing the 2',5'-UUCC loop and, in fact, they may be replaced altogether (ribose--> deoxyribose) without affecting stability. The results broaden our understanding of the behavior of highly stable (UUCG) hairpin loops and how they respond to structural perturbation of the loop-closing base pairs.     

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.     

Molecular dynamics simulations of the denaturation and refolding of an RNA tetraloop.

Tetraloops are very abundant structural elements of RNA that are formed by four nucleotides in a hairpin loop which is closed by a double stranded helical stem with some Watson-Crick base pairs. A tetraloop r(GCGAAGGC) was identified from the crystal structure of the central domain of 16S rRNA (727-730) in the Thermus thermophilus 30S ribosomal complex. The crystal structure of the 30S complex includes a total of 104 nucleotides from the central domain of the 16S rRNA and three ribosomal proteins S6, S15 and S18. Independent biochemical experiments have demonstrated that protein S15 plays the role in initiating the formation of the central domain of this complex. In the crystal, the tetraloop interacts with the protein S15 at two sites: one of them is associated with hydrogen bond interactions between residue His50 and nucleotide G730, and the other is associated with the occurrence of residue Arg53 beside A728. This paper uses molecular dynamics (MD) simulations to investigate the protein-dependent structural stability of the tetraloop and demonstrates the folding pathway of this tetraloop via melting denaturation and its subsequent refolding. Three important results are derived from these simulations: (i) The stability of nucleotide A728 appears to be protein dependent. Without the interaction with S15, A728 flips away from stacking with A729. (ii) The melting temperature demonstrated by the simulations is analogous to the results of thermodynamic experiments. In addition, the simulated folding of the tetraloop is stepwise: the native shape of the backbone is formed first; this is then followed by the formation of the Watson- Crick base pairs in the stem; and finally the hydrogen bonds and base stacking in the loop are formed. (iii) The tetraloop structure is similar to the crystal structure at salt concentrations of 0.1 M and 1.0 M used for the simulations, but the refolded structure at 0.1 M salt is more comparable to the crystal structure than at 1.0 M. The results from the simulations using both the Generalized Born continuum model and explicit solvent model (Particle Mesh Ewald) generate a similar pathway for unfolding/refolding of the tetraloop.