Solution structure of a GAAA tetraloop receptor RNA.

The GAAA tetraloop receptor is an 11-nucleotide RNA sequence that participates in the tertiary folding of a variety of large catalytic RNAs by providing a specific binding site for GAAA tetraloops. Here we report the solution structure of the isolated tetraloop receptor as solved by multidimensional, heteronuclear magnetic resonance spectroscopy. The internal loop of the tetraloop receptor has three adenosines stacked in a cross-strand or zipper-like fashion. This arrangement produces a high degree of base stacking within the asymmetric internal loop without extrahelical bases or kinking the helix. Additional interactions within the internal loop include a U. U mismatch pair and a G.U wobble pair. A comparison with the crystal structure of the receptor RNA bound to its tetraloop shows that a conformational change has to occur upon tetraloop binding, which is in good agreement with previous biochemical data. A model for an alternative binding site within the receptor is proposed based on the NMR structure, phylogenetic data and previous crystallographic structures of tetraloop interactions.     

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.     

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.     

Extending the family of UNCG-like tetraloop motifs: NMR structure of a CACG tetraloop from coxsackievirus B3

Stable RNA tetraloop motifs are found frequently in biologically active RNAs. These motifs carry out a wide variety of functions in RNA folding, in RNA-RNA and RNA-protein interactions. A great deal of knowledge about the structures and functions of tetraloop motifs has accumulated largely due to intensive theoretical, biochemical, and biophysical studies on three most frequently occurring families of tetraloop sequences, namely, the cUNCGg, the cGNRAg, and the gCUUGc sequences. Our knowledge surely is not exhaustive, and efforts are still being made to gain a better understanding. Here we report the NMR structure of a uCACGg tetraloop that occurs naturally within the cloverleaf RNA structure of the 5'-UTR of coxsackievirus B3. This tetraloop is the major determinant for interaction between the cloverleaf RNA and viral 3C protease, which is an essential part of a ribonucleoprotein complex that plays a critical role in the regulation of viral translation and replication. Our structure shows that the CACG tetraloop is closed by a wobble U.G base pair. The structure of the CACG tetraloop is stabilized by extensive base stacking and hydrogen bonding interactions strikingly similar to those previously reported for the cUUCGg tetraloop. Identification of these hallmark structural features strongly supports the existence of an extended YNCG tetraloop family. The U.G base pair closing the stem and the A residue in the loop introduce some small structural and themodynamic distinctions from the canonical cUUCGg tetraloop that may be important for recognition by the viral 3C protease.     

Mutational and structural analysis of stem-loop IIIC of the hepatitis C virus and GB virus B internal ribosome entry sites

Translation of the open reading frames (ORF) of the hepatitis C virus (HCV) and closely related GB virus B (GBV-B) genomes is driven by internal ribosome entry site (IRES) elements located within the 5' non-translated RNA. The functioning of these IRES elements is highly dependent on primary and higher order RNA structures. We present here the solution structures of a common, critical domain within each of these IRESs, stem-loop IIIc. These ten-nucleotide hairpins have nearly identical sequences and similar overall tertiary folds. The final refined structure of each shows a stem with three G:C base-pairs and a novel tetraloop fold. Although the bases are buckled, the first and fourth nucleotides of both tetraloops form a Watson-Crick type base-pair, while the apical nucleotides are located in the major groove where they adopt C(2)-endo sugar puckering with B-form geometry. No hydrogen bonding interactions were observed involving the two apical residues of the tetraloop. Stability of the loops appears to be derived primarily from the stacking of bases, and the hydrogen bonding between the fourth and seventh residues. Mutational analysis shows that the primary sequence of stem-loop IIIc is important for IRES function and that the stem and first and fourth nucleotides of the tetraloop contribute to the efficiency of internal ribosome entry. Base-pair formation between these two positions is essential. In contrast, the apical loop nucleotides differ between HCV and GBV-B, and substitutions in this region of the hairpin are tolerated without major loss of function.     

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.     

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

Abstract

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 gly- cosyl 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.     

Common and distinctive features of GNRA tetraloops based on a GUAA tetraloop structure at 1.4 A resolution

GNRA tetraloops (N is A, C, G, or U; R is A or G) are basic building blocks of RNA structure that often interact with proteins or other RNA structural elements. Understanding sequence-dependent structural variation among different GNRA tetraloops is an important step toward elucidating the molecular basis of specific GNRA tetraloop recognition by proteins and RNAs. Details of the geometry and hydration of this motif have been based on high-resolution crystallographic structures of the GRRA subset of tetraloops; less is known about the GYRA subset (Y is C or U). We report here the structure of a GUAA tetraloop determined to 1.4 A resolution to better define these details and any distinctive features of GYRA tetraloops. The tetraloop is part of a 27-nt structure that mimics the universal sarcin/ricin loop from Escherichia coli 23S ribosomal RNA in which a GUAA tetraloop replaces the conserved GAGA tetraloop. The adenosines of the GUAA tetraloop form an intermolecular contact that is a commonplace RNA tertiary interaction called an A-minor motif. This is the first structure to reveal in great detail the geometry and hydration of a GUAA tetraloop and an A-minor motif. Comparison of tetraloop structures shows a common backbone geometry for each of the eight possible tetraloop sequences and suggests a common hydration. After backbone atom superposition, equivalent bases from different tetraloops unexpectedly depart from coplanarity by as much as 48 degrees. This variation displaces the functional groups of tetraloops implicated in protein and RNA binding, providing a recognition feature.     

UNAC tetraloops: to what extent do they mimic GNRA tetraloops?

The structures of four small RNAs each containing a different version of the UNAC loop were determined in solution using NMR spectroscopy and restrained molecular dynamics. The UMAC tetraloops (where M is A or C) exhibited a typical GNRA fold including at least one hydrogen bond between the first U and fourth C. In contrast, UGAC and UUAC tetraloops have a different orientation of the first and fourth residues, such that they do not closely mimic the GNRA fold. Although the UMAC tetraloops are excellent structural mimics of the GNRA tetraloop backbone, sequence comparisons typically do not reveal co‐variation between the two loop types. The limited covariation is attributed to differences in the location of potential hydrogen bond donors and acceptors as a result of the replacement of the terminal A of GNRA with C in the UMAC version. Thus, UMAC loops do not readily form the common GNRA tetraloop‐receptor interaction. The loop at positions 863‐866 in E. coli 16S ribosomal RNA appears to be a major exception. However, in this case the GNRA loop does not in fact engage in the usual base to backbone tertiary interactions. In summary, UMAC loops are not just an alternative sequence version of the GNRA loop family, but instead they expand the types of interactions, or lack thereof, that are possible. From a synthetic biology perspective their inclusion in an artificial RNA may allow the establishment of a stable loop structure while minimizing unwanted long range interactions or permitting alternative long‐range interactions. © 2012 Wiley Periodicals, Inc. Biopolymers 97: 617–628, 2012.     

Structure of the histone mRNA hairpin required for cell cycle regulation of histone gene expression

Expression of replication-dependent histone genes requires a conserved hairpin RNA element in the 3' untranslated regions of poly(A)-less histone mRNAs. The 3' hairpin element is recognized by the hairpin-binding protein or stem-loop-binding protein (HBP/SLBP). This protein-RNA interaction is important for the endonucleolytic cleavage generating the mature mRNA 3' end. The 3' hairpin and presumably HBP/SLBP are also required for nucleocytoplasmic transport, translation, and stability of histone mRNAs. RNA 3' processing and mRNA stability are both regulated during the cell cycle. Here, we have determined the three-dimensional structure of a 24-mer RNA comprising a mammalian histone RNA hairpin using heteronuclear multidimensional NMR spectroscopy. The hairpin adopts a novel UUUC tetraloop conformation that is stabilized by base stacking involving the first and third loop uridines and a closing U-A base pair, and by hydrogen bonding between the first and third uridines in the tetraloop. The HBP interaction of hairpin RNA variants was analyzed in band shift experiments. Particularly important interactions for HBP recognition are mediated by the closing U-A base pair and the first and third loop uridines, whose Watson-Crick functional groups are exposed towards the major groove of the RNA hairpin. The results obtained provide novel structural insight into the interaction of the histone 3' hairpin with HBP, and thus the regulation of histone mRNA metabolism.     

A conserved major groove antideterminant for Saccharomyces cerevisiae RNase III recognition

Rnt1p, the only known Saccharomyces cerevisiae RNase III double-stranded RNA endonuclease, plays important roles in the processing of precursors of ribosomal RNAs and small nuclear and nucleolar RNAs and in the surveillance of unspliced pre-mRNAs. Specificity of cleavage by Rnt1p relies on the presence of RNA tetraloop structures with the consensus sequence AGNN at the top of the target dsRNA. The sequences of 79 fungal RNase III substrates were inspected to identify additional conserved sequence elements or antideterminants that may contribute to Rnt1p recognition of the double-stranded RNA. Surprisingly, U-A sequences at the base pair adjacent to the conserved terminal tetraloop (closing base pair) were found to be absent from all but one inspected sequence. Analysis of chemically modified variants of the closing base pair showed that the presence of exocyclic groups in the major groove of purines 3' to the last nucleotide of the tetraloop inhibits Rnt1p cleavage without strongly inhibiting Rnt1p binding. We propose that these groups interfere with the recognition of the RNA substrate by the catalytic domain of Rnt1p. These results identify exocyclic groups of purines in the major groove downstream of the tetraloop as a major antideterminant in S. cerevisiae RNase III activity, and suggest a rationale for their apparent counter selection in RNA processing sites.     

The application of cluster analysis in the intercomparison of loop structures in RNA

We have developed a computational approach for the comparison and classification of RNA loop structures. Hairpin or interior loops identified in atomic resolution RNA structures were intercompared by conformational matching. The root-mean-square deviation (RMSD) values between all pairs of RNA fragments of interest, even if from different molecules, are calculated. Subsequently, cluster analysis is performed on the resulting matrix of RMSD distances using the unweighted pair group method with arithmetic mean (UPGMA). The cluster analysis objectively reveals groups of folds that resemble one another. To demonstrate the utility of the approach, a comprehensive analysis of all the terminal hairpin tetraloops that have been observed in 15 RNA structures that have been determined by X-ray crystallography was undertaken. The method found major clusters corresponding to the well-known GNRA and UNCG types. In addition, two tetraloops with the unusual primary sequence UMAC (M is A or C) were successfully assigned to the GNRA cluster. Larger loop structures were also examined and the clustering results confirmed the occurrence of variations of the GNRA and UNCG tetraloops in these loops and provided a systematic means for locating them. Nineteen examples of larger loops that closely resemble either the GNRA or UNCG tetraloop were found in the large ribosomal RNAs. When the clustering approach was extended to include all structures in the SCOR database, novel relationships were detected including one between the ANYA motif and a less common folding of the GAAA tetraloop sequence.     

Comprehensive survey and geometric classification of base triples in RNA structures

Base triples are recurrent clusters of three RNA nucleobases interacting edge-to-edge by hydrogen bonding. We find that the central base in almost all triples forms base pairs with the other two bases of the triple, providing a natural way to geometrically classify base triples. Given 12 geometric base pair families defined by the Leontis-Westhof nomenclature, combinatoric enumeration predicts 108 potential geometric base triple families. We searched representative atomic-resolution RNA 3D structures and found instances of 68 of the 108 predicted base triple families. Model building suggests that some of the remaining 40 families may be unlikely to form for steric reasons. We developed an on-line resource that provides exemplars of all base triples observed in the structure database and models for unobserved, predicted triples, grouped by triple family, as well as by three-base combination (http://rna.bgsu.edu/Triples). The classification helps to identify recurrent triple motifs that can substitute for each other while conserving RNA 3D structure, with applications in RNA 3D structure prediction and analysis of RNA sequence evolution.     

A novel family of RNA tetraloop structure forms the recognition site for Saccharomyces cerevisiae RNase III.

RNases III are a family of double-stranded RNA (dsRNA) endoribonucleases involved in the processing and decay of a large number of cellular RNAs as well as in RNA interference. The dsRNA substrates of Saccharomyces cerevisiae RNase III (Rnt1p) are capped by tetraloops with the consensus sequence AGNN, which act as the primary docking site for the RNase. We have solved the solution structures of two RNA hairpins capped by AGNN tetraloops, AGAA and AGUU, using NMR spectroscopy. Both tetraloops have the same overall structure, in which the backbone turn occurs on the 3' side of the syn G residue in the loop, with the first A and G in a 5' stack and the last two residues in a 3' stack. A non-bridging phosphate oxygen and the universal G which are essential for Rnt1p binding are strongly exposed. The compared biochemical and structural analysis of various tetraloop sequences defines a novel family of RNA tetraloop fold with the consensus (U/A)GNN and implicates this conserved structure as the primary determinant for specific recognition of Rnt1p substrates.     

Molecular analysis of the role of IRES stem-loop V in replicative capacities and translation efficiencies of Coxsackievirus B3 mutants

Coxsackievirus B3 (CVB3) is a principal viral cause of acute myocarditis in humans and has been implicated in the pathogenesis of dilated cardiomyopathy. The natural genetic determinants of cardiovirulence for CVB3 have not been identified, although using strains engineered in the laboratory, it has been demonstrated elsewhere that, for several wild-type CB3 strains, the primary molecular determinant of cardiovirulence phenotype localizes to the 5′ nontranslated region (5′NTR) and capsid. Stable RNA tetraloop motifs are found frequently in biologically active RNAs. These motifs carry out a wide variety of functions in RNA folding, in RNA–RNA and RNA–protein interactions. A great deal of knowledge about the structures and functions of tetraloop motifs has accumulated largely due to intensive theoretical, biochemical, and biophysical studies on one most frequently occurring family of tetraloop sequences, namely, the GNRA sequence, especially the GNAA sequence conserved in all enteroviruses. Here in this study, through construction of CVB3 chimeric mutants, the predicted stem loop (SL) V within the 5′NTR has been identified as important in determining viral cardiovirulence. Replication assays in HeLa cell monolayers revealed that wild-type CVB3 virus and two of the six mutants constructed here grow efficiently, whereas other mutant viruses replicate poorly. Furthermore, the in vitro translation products from these mutants and wild-type CVB3, demonstrated that the two mutants who replicate efficiently, translated at relatively equivalent amount than the wild-type. However, other mutants demonstrated a low efficiency in their production of protein when translated in a Rabbit Reticulocytes Lysats.     

The major HIV-1 packaging signal is an extended bulged stem loop whose structure is altered on interaction with the Gag polyprotein

The major packaging signal of human immunodeficiency virus type 1 (HIV-1) RNA has been localised to the region 3' to the major splice donor within the leader sequence. Secondary structural studies for this region of the HIV-1 genome have shown the existence of a stem-loop structure capped by a purine-rich tetraloop. Extensive mapping data presented here lead to the complete characterisation of the structure of the stem-loop, including a new purine-rich internal loop in the lower part of the structure and the previously established GGAG tetraloop at its tip. Biochemical analysis reveals that both internal loop and tetraloop are primary sites for interaction with Gag polyprotein, and that binding of Gag protein leads to a conformational change which alters the RNA structure. NMR spectroscopy has been used to determine the three-dimensional structure of this complete stem-loop structure. The structural analysis reveals a significant difference between the apical part of the stem-loop structure, which adopts a well-defined conformation, and the purine-rich internal loop, which is instead very flexible. In contrast to what is generally observed for internal loop structures in RNA, this region of the encapsidation signal adopts a structure lacking stable interstrand interactions capable of stabilising a unique conformation. We suggest that the stem-loop structure represents a nucleation site for Gag protein binding, and that the protein exploits the flexibility of the internal loop to initiate the unwinding of the structure with successive addition of Gag molecules interacting with the RNA and each other through conserved I (interaction) domains.     

Structure of an AAGU tetraloop and its contribution to substrate selection by yeast RNase III

RNase III enzymes are a highly conserved family of proteins that specifically cleave double-stranded RNA (dsRNA). These proteins are involved in a variety of cellular functions, including the processing of many non-coding RNAs, mRNA decay, and RNA interference. In yeast Rnt1p, a dsRNA-binding domain (dsRBD) recognizes its substrate by interacting with stems capped with conserved AGNN tetraloops. The enzyme uses the tetraloop to cut 14nt to 16nt away into the stem in a ruler-like mechanism. The solution structure of Rnt1p dsRBD complexed to one of its small nucleolar (sno) RNA substrate revealed non-sequence-specific contacts with the sugar-phosphate backbone in the minor groove of the AGNN fold and the two non-conserved tetraloop nucleotides. Recently, a new form of Rnt1p substrates lacking the conserved AGNN sequence but instead harboring an AAGU tetraloop was found at the 5' end of snoRNA 48 precursor. Here, we report the solution structure of this hairpin capped with an AAGU tetraloop. Some of the stacking interactions and the position of the turn in the sugar-phosphate backbone are similar to the one observed in the AGNN loop structure; however, the AAGU sequence adopts a different conformation. The most striking difference was found at the 3' end of the loop where Rnt1p interacts with AGNN substrates. The last nucleotide is extruded from the AAGU tetraloop structure in contrast to the compact AGNN fold. The AAGU hairpin structure suggests that Rnt1p recognizes substrates with different tetraloop structures, indicating that the structural repertoire specifically recognized by Rnt1p is larger than previously anticipated.     

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.     

A GCUA tetranucleotide loop found in the poliovirus oriL by in vivo SELEX (un)expectedly forms a YNMG-like structure: Extending the YNMG family with GYYA

The cloverleaf structure in the 5'-untranslated region of enterovirus RNA that regulates viral RNA replication contains an evolutionarily conserved YNMG tetraloop closed by a Y-G base pair. This loop is believed to interact specifically with the viral protease 3C. To further characterize the specificity of this interaction, the tetraloop and two flanking base pairs of the poliovirus RNA were randomized, and viable viral clones were obtained using in vivo SELEX. Among many different mutants with the canonical YNMG sequences to be described elsewhere, a large-plaque-forming clone contained a deviating uGCUAg sequence. The NMR structure of a small hairpin capped with uGCUAg that we present here shows that the GCUA tetraloop adopts a novel fold, which is highly similar to that of the YNMG tetraloop with common stacking properties and hydrogen-bond interactions including an unusual syn conformation of the adenosine. Thermodynamic studies show moderate stabilities of hairpins with canonical YNMG and the novel GCUA loops, which, together with the similarity of spatial structures, illustrates that the tetraloop structure itself is crucial for the RNA-protein interaction required for the viral replication. A re-evaluation of the ribosomal secondary structure database reveals a hairpin containing a GCUA loop, which covaries with YNMG and is involved in a tertiary interaction, and in the 50S ribosomal subunit from Haloarcula marismortui the structurally comparable apex of stem-loop 35a is a recognition site for protein L2. These observations show a more general occurrence and importance of the so-far unrecognized GYYA hairpin loops.     

The structure of the isolated, central hairpin of the HDV antigenomic ribozyme: novel structural features and similarity of the loop in the ribozyme and free in solution.

The structure of an RNA hairpin containing a seven-nucleotide loop that is present in the self-cleaving sequence of hepatitis delta virus antigenomic RNA was determined by high resolution NMR spectroscopy. The loop, which is composed of only one purine and six pyrimidines, has a suprisingly stable structure, mainly supported by sugar hydroxyl hydrogen bonds and base-base and base-phosphate stacking interactions. Compared with the structurally well-determined, seven-membered anticodon loop in tRNA, the sharp turn which affects the required 180 degrees change in direction of the sugar-phosphate backbone in the loop is shifted one nucleotide in the 3' direction. This change in direction can be characterized as a reversed U-turn. It is expected that the reversed U-turn may be found frequently in other molecules as well. There is evidence for a new non-Watson-Crick UC base pair formed between the first and the last residue in the loop, while most of the other bases in the loop are pointing outwards making them accessible to solvent. From chemical modification, mutational and photocrosslinking studies, a similar picture develops for the structure of the hairpin in the active ribozyme indicating that the loop structure in the isolated hairpin and in the ribozyme is very similar.