Solution conformation of a bulged adenosine base in an RNA duplex by relaxation matrix refinement

Bulges are common structural motifs in RNA secondary structure and are thought to play important roles in RNA-protein and RNA-drug interactions. Adenosine bases are the most commonly occurring unpaired base in double helical RNA secondary structures. The solution conformation and dynamics of a 25-nucleotide RNA duplex containing an unpaired adenosine, r(GGCAGAGUGCCGC): r(GCGGCACCUGCC) have been studied by NMR spectroscopy and MORASS iterative relaxation matrix structural refinement. The results show that the bulged adenosine residue stacks into the RNA duplex with little perturbation around the bulged region. Most of the bases in the RNA duplex adopt C(3)'-endo conformation, exhibiting the N-type sugar pucker as found in the A form helices. The sugars of the bulged residue and the 5' flanking residue to it are found to exhibit C(2)'-endo conformation. None of the residues are in syn conformation.     

Bulged adenosine influence on the RNA duplex conformation in solution

The RNA single bulge motif is an unpaired residue within a strand of several complementary base pairs. To gain insight into structural changes induced by the presence of the adenosine bulge on RNA duplex, the solution structures of RNA duplex containing a single adenine bulge (5'-GCAGAAGAGCG-3'/5'-CGCUCUCUGC-3') and a reference duplex with all Watson-Crick base pairs (5'-GCAGAGAGCG-3'/5'-CGCUCUCUGC-3') have been determined by NMR spectroscopy. The reference duplex structure is a regular right-handed helix with all of the attributes of an A-type helix. In the bulged duplex, single adenine bulge stacks into the helix, and the bulge region forms a well-defined structure. Both structures were analyzed by the use of calculated helical parameters. Distortions induced by the accommodation of unpaired residue into the helical structure propagate over the entire structure and are manifested as the reduced base pairs inclination and x-displacement. Intrahelical position of bulged adenine A5 is stabilized by efficient stacking with 5'-neighboring residues G4.     

Solution structure of the SL1 RNA of the M1 double-stranded RNA virus of Saccharomyces cerevisiae

The 20-nucleotide SL1 VBS RNA, 5'-GGAGACGC[GAUUC]GCGCUCC (bulged A underlined and loop bases in brackets), plays a crucial role in viral particle binding to the plus strand and packaging of the RNA. Its structure was determined by NMR spectroscopy. Structure calculations gave a precisely defined structure, with an average pairwise root mean square deviation (RMSD) of 1.28 A for the entire molecule, 0.57 A for the loop region (C8-G14), and 0.46 A for the bulge region (G4-G7, C15-C17). Base stacking continues for three nucleotides on the 5' side of the loop. The final structure contains a single hydrogen bond involving the guanine imino proton and the carbonyl O(2) of the cytosine between the nucleotides on the 5' and 3' ends of the loop, although they do not form a Watson-Crick base pair. All three pyrimidine bases in the loop point toward the major groove, which implies that Cap-Pol protein may recognize the major groove of the SL1 loop region. The bulged A5 residue is stacked in the stem, but nuclear Overhauser enhancements (NOEs) suggest that A5 spends part of the time in the bulged-out conformation. The rigid conformation of the upper stem and loop regions may allow the SL1 VBS RNA to interact with Cap-Pol protein without drastically changing its own conformation.     

Hydration of [d(CGC)r(aaa)d(TTTGCG)](2)

We have studied the hydration and dynamics of RNA C2'-OH in a DNA. RNA hybrid chimeric duplex [d(CGC)r(aaa)d(TTTGCG)](2). Long-lived water molecules with correlation time tau(c) larger than 0.3 ns were found close to the RNA adenine H2 and H1' protons in the hybrid segment. A possible long-lived water molecule was also detected close to the methyl group of 7T in the RNA-DNA junction but not to the other two thymine bases (8T and 9T). This result correlates with the structural studies that only DNA residue 7T in the RNA-DNA junction adopts an O4'-endo sugar conformation (intermediate between B-form and A-form), while the other DNA residues including 3C in the DNA-RNA junction, adopt C1'-exo or C2'-endo conformations (in the B-form domain). Based on the NOE cross-peak patterns, we have found that RNA C2'-OH tends to orient toward the O3' direction, forming a possible hydrogen bond with the 3'-phosphate group. The exchange rates for RNA C2'-OH were found to be around 5-20 s(-1), compared to 26.7(+/-13.8) s(-1) reported previously for the other DNA.RNA hybrid duplex. This slow exchange rate may be due to the narrow minor groove width of [d(CGC)r(aaa)d(TTTGCG)](2), which may trap the water molecules and restrict the dynamic motion of hydroxyl protons. The distinct hydration patterns of the RNA adenine H2 and H1' protons and the DNA 7T methyl group in the hybrid segment, as well as the orientation and dynamics of the RNA C2'-OH protons, may provide a molecular basis for further understanding the structure and recognition of DNA.RNA hybrid and chimeric duplexes.     

Crystal structure of an RNA duplex r(gugucgcac)(2) with uridine bulges.

The crystal structure of a nonamer RNA duplex with a uridine bulge in each strand, r(gugucgcac)(2), was determined at 1.4 A resolution. The structure was solved by multiple anomalous diffraction phasing method using a three-wavelength data set collected at the Advanced Protein Source and refined to a final R(work)/R(free) of 21.2 %/23.4 % with 33,271 independent reflections (Friedel pairs unmerged). The RNA duplex crystallized in the tetragonal space group P4(1)22 with two independent molecules in the asymmetric unit. The unit cell dimensions are a=b=47.18 A and c=80.04 A. The helical region of the nonamer adopts the A-form conformation. The uridine bulges assume similar conformations, with uracils flipping out and protruding into the minor groove. The presence of the bulge induces very large twist angles (approximately +50 degrees) between the base-pairs flanking the bulges while causing profound kinks in the helix axis at the bulges. This severe twist and the large kink in turn produces a very narrow major groove at the middle of the molecule. The ribose sugars of the guanosines before the bulges adopt the C2'-endo conformation while the rest, including the bulges, are in the C3'-endo conformation. The intrastrand phosphate-phosphate (P-P) distance of the phosphate groups flanking the bulges (approximately 4.4 A) are significantly shorter than the average P-P distance in the duplex (6.0 A). This short distance between the two phosphate groups brings the non-bridging oxygen atoms close to each other where a calcium ion is bound to each strand. The calcium ions in molecule 1 are well defined while the calcium ions in molecule 2 are disordered.     

NMR structure of an antisense DNA.RNA hybrid duplex containing a 3'-CH(2)N(CH(3))-O-5' or an MMI backbone linker.

The solution structure of an antisense DNA.RNA hybrid duplex, d(CGCGTT-MMI-TTGCGC).r(GCGCAAAACGCG) (designated R4), containing an MMI backbone linker [3'-CH(2)N(CH(3))-O5'], is elucidated. The structural details of the MMI linker, its structural effects on the neighboring residues, and the molecular basis of the MMI effects are examined. The lipophilic N-methyl group of MMI is peripheral to the helix, assuming a conformation that is most stable with regard to the N-O torsion angle. The MMI linker promotes a 3'-endo conformation for the sugar moieties at both 3'- and 5'-adjacent positions and a backbone kink involving distant residues along the 3'-direction. Comparison of R4 with other analogous hybrid duplexes previously studied in this laboratory reveals a new family of low-energy helical conformations that can be accommodated in stable duplexes and a common feature of C3'-modified sugars for adopting a C3'-endo pucker. The results of these studies emphasize the interplay of several factors that govern the formation of stable hybrid duplexes and provide a basis for the understanding of the biological role of the MMI modifications, which are important building blocks for a family of promising chimeric antisense oligonucleotides.     

Crystal structure of a bulged RNA tetraplex at 1.1 a resolution: implications for a novel binding site in RNA tetraplex

Bulges are an important structural motif in RNA and can be used as recognition and interaction sites in RNA-protein interaction and RNA-RNA interaction. Here we report the first crystal structure of a bulged RNA tetraplex at 1.1 A resolution. The hexamer r(U)(BrdG)r(UGGU) forms a parallel tetraplex with the uridine sandwiched by guanines bulging out. The bulged uridine adopts the syn glycosidic conformation and its O2 and N3 atoms face outwards, serving as an effective recognition and interaction site. The bulge formation both widens the groove width and changes the groove hydrogen-bonding pattern on its 5' side. However, the bulge does not make any bends or kinks in the tetraplex structure. The present study demonstrates the dramatic difference between uridine and guanine in forming tetraplex structure. In addition, both G(syn) tetrad and G(anti) tetrad have been observed. They display the same base-pairing pattern and similar C1'-C1' distance but different hydrogen-bonding patterns in the groove.     

Conformational analysis of single-base bulges in A-form DNA and RNA using a hierarchical approach and energetic evaluation with a continuum solvent model.

The analysis and prediction of non-canonical structural motifs in RNA is of great importance for an understanding of the function and design of RNA structures. A hierarchical method has been employed to generate a large variety of sterically possible conformations for a single-base adenine bulge structure in A -form DNA and RNA. A systematic conformational search was performed on the isolated bulge motif and neighboring nucleotides under the constraint to fit into a continuous helical structure. These substructures were recombined with double-stranded DNA or RNA. Energy minimization resulted in more than 300 distinct bulge conformations. Energetic evaluation using a solvation model based on the finite-difference Poisson-Boltzmann method identified three basic classes of low-energy structures. The three classes correspond to conformations with the bulge base stacked between flanking nucleotides (I), location of the bulge base in the minor groove (II) and conformations with a continuous stacking of the flanking helices and a looped out bulge base (III). For the looped out class, two subtypes (IIIa and IIIb) with different backbone geometries at the bulge site could be distinguished. The conformation of lowest calculated energy was a class I structure with backbone torsion angles close to those in standard A -form RNA. Conformations very close to the extra-helical looped out bulge structure determined by X-ray crystallography were also among the low-energy structures. In addition, topologies observed in other experimentally determined bulge structures have been found among low-energy conformers. The implicit solvent model was further tested by comparing an uridine and adenine bulge flanked by guanine:cytosine base-pairs, respectively. In agreement with the experimental observation, a looped out form was found as the energetically most favorable form for the uridine bulge and a stacked conformation in case of the adenine bulge. The inclusion of solvation effects especially electrostatic reaction field contributions turned out to be critically important in order to select realistic low-energy bulge structures from a large number of sterically possible conformations. The results indicate that the approach might be useful to model the three-dimensional structure of non-canonical motifs embedded in double-stranded RNA, in particular, to restrict the number of possible conformations to a manageable number of conformers with energies below a certain threshold.     

High-resolution NMR study of a synthetic DNA-RNA hybrid dodecamer containing the consensus pribnow promoter sequence: d(CGTTATAATGCG).r(CGCAUUAUAACG)

The nonsymmetrical double-helical hybrid dodecamer d(CGTTATAATGCG).r(CGCAUUAUAACG) was synthesized with solid-phase phosphoramidite methods and studied by high-resolution 2D NMR. The imino protons were assigned by one-dimensional nuclear Overhauser methods. All the base protons and H1', H2', H2", H3', and H4' sugar protons of the DNA strand and the base protons, H1', H2', and most of the H3'-H4' protons of the RNA strand were assigned by 2D NMR techniques. The well-resolved spectra allowed a qualitative analysis of relative proton-proton distances in both strands of the dodecamer. The chemical shifts of the hybrid duplex were compared to those of the pure DNA double helix with the same sequence (Wemmer et al., 1984). The intrastrand and cross-strand NOEs from adenine H2 to H1' resonances of neighboring base pairs exhibited characteristic patterns that were very useful for checking the spectral assignments, and their highly nonsymmetric nature reveals that the conformations of the two strands are quite different. Detailed analysis of the NOESY and COSY spectra, as well as the chemical shift data, indicate that the RNA strand assumes a normal A-type conformation (C3'-endo) whereas the DNA strand is in the general S domain but not exactly in the normal C2'-endo conformation. The overall structure of this RNA-DNA duplex is different from that reported for hybrid duplexes in solution by other groups (Reid et al., 1983a; Gupta et al., 1985) and is closer to the C3'-endo-C2'-endo hybrid found in poly(dA).poly(dT) and poly(rU).poly(dA) in the fiber state (Arnott et al., 1983, 1986).     

Role of conserved nucleotides in building the 16S rRNA binding site of E. coli ribosomal protein S8.

Ribosomal protein S8 specifically recognizes a helical and irregular region of 16S rRNA that is highly evolutionary constrained. Despite its restricted size, the precise conformation of this region remains a question of debate. Here, we used chemical probing to analyze the structural consequences of mutations in this RNA region. These data, combined with computer modelling and previously published data on protein binding were used to investigate the conformation of the RNA binding site. The experimental data confirm the model in which adenines A595, A640 and A642 bulge out in the deep groove. In addition to the already proposed non canonical U598-U641 interaction, the structure is stabilized by stacking interactions (between A595 and A640) and an array of hydrogen bonds involving bases and the sugar phosphate backbone. Mutations that alter the ability to form these interdependent interactions result in a local destabilization or reorganization. The specificity of recognition by protein S8 is provided by the irregular and distorted backbone and the two bulged adenines 640 and 642 in the deep groove. The third adenine (A595) is not a direct recognition site but must adopt a bulged position. The U598-U641 pair should not be directly in contact with the protein.     

The crystal structure of the RNA/DNA hybrid r(GAAGAGAAGC). d(GCTTCTCTTC) shows significant differences to that found in solution.

The crystal structure of the RNA/DNA hybrid r(GAAGAGAAGC). d(GCTTCTCTTC) has been solved and refined at 2.5 A resolution. The refinement procedure converged at R = 0.181 for all reflections in the range 20.0-2.5 A. In the crystal, the RNA/DNA hybrid duplex has an A' conformation with all but one of the nucleotide sugar moieties adopting a C3'- endo (N) conformation. Both strands in the double helix adopt a global conformation close to the A-form and the width of the minor groove is typical of that found in the crystal structures of other A-form duplexes. However, differences are observed between the RNA and DNA strands that make up the hybrid at the local level. In the central portion of the duplex, the RNA strand has backbone alpha, beta and gamma torsion angles that alternate between the normal gauche -/ trans / gauche + conformation and an unusual trans / trans / trans conformation. Coupled with this so-called 'alpha/gamma flipping' of the backbone torsion angles, the distance between adjacent phosphorous atoms on the RNA strand systematically varies. Neither of these phenomena are observed on the DNA strand. The structure of the RNA/DNA hybrid presented here differs significantly from that found in solution for this and other sequences. Possible reasons for these differences and their implications for the current model of RNase H activity are discussed.     

Solution structure of a five-adenine bulge loop within a DNA duplex.

The three-dimensional solution structure of a DNA molecule of the sequence 5'-d(GCATCGAAAAAGCTACG)-3' paired with 5'-d(CGTAGCCGATGC)-3' containing a five-adenine bulge loop (dA(5)-bulge) between two double helical stems was determined by 2D (1)H and (31)P NMR, infrared, and Raman spectroscopy. The DNA in both stems adopt a classical B-form double helical structure with Watson-Crick base pairing and C2'-endo sugar conformation. In addition, the two dG/dC base pairs framing the dA(5)-bulge loop are formed and are stable at least up to 30 degrees C. The five adenine bases of the bulge loop are localized at intrahelical positions within the double helical stems. Stacking on the double helical stem is continued for the first four 5'-adenines in the bulge loop. The total rise (the height) of these four stacked adenines roughly equals the diameter of the double helical stem. The stacking interactions are broken between the last of these four 5'-adenines and the fifth loop adenine at the 3'-end. This 3'-adenine partially stacks on the other stem. The angle between the base planes of the two nonstacking adenines (A10 and A11) in the bulge loop reflects the kinking angle of the global DNA structure. The neighboring cytosines opposite the dA(5)-bulge (being parts of the bulge flanking base pairs) do not stack on one another. This disruption of stacking is characterized by a partial shearing of these bases, such that certain sequential NOEs for this base step are preserved. In the base step opposite the loop, an extraordinary hydrogen bond is observed between the phosphate backbone of the 5'-dC and the amino proton of the 3'-dC in about two-thirds of the conformers. This hydrogen bond probably contributes to stabilizing the global DNA structure. The dA(5)-bulge induces a local kink into the DNA molecule of about 73 degrees (+/-11 degrees ). This kinking angle and the mutual orientation of the two double helical stems agree well with results from fluorescence resonance energy transfer measurements of single- and double-bulge DNA molecules.     

Molecular structures of two new anti-HIV nucleoside analogs: 9-(2,3-dideoxy-2-fluoro-beta-D-threo-pentofuranosyl)adenine and 9-(2,3-dideoxy-2-fluoro-beta-D-threo-pentofuranosyl)hypoxanthine.

The x-ray crystal structures of two new anti-HIV compounds, 9-(2,3-dideoxy-2-fluoro-beta-D-threo-pentofuranosyl)adenine (2'-F-dd-araA) and 9-(2,3-dideoxy-2-fluoro-beta-D-threo- pentofuranosyl)hypoxanthine (2'-F-dd-aral), have been determined at two temperatures. Both crystals are in the space group P2(1)2(1)2(1), and their structures were solved by direct methods. Least-squares refinement produced final R-factors of 0.027 for the 2'-F-dd-araA structure and of 0.044 for the 2'-F-dd-aral structure, respectively. The latter structure contains a two-fold disordered conformation of the sugar moiety. All three conformers (one for 2'-F-dd-araA and two for 2'-F-dd-aral) adopt an anti chi CN glycosyl torsion angle. The sugar in the 2'-F-dd-araA structure has a C2'-endo pucker conformation, whereas the sugar in the 2'-F-dd-aral structure has a mixture of C2'-endo and C3'-endo pucker conformations. When the sugar adopts the C2'-endo conformation, the torsion angle about the C4'-C5' bond is in a transgauche+ conformation. In contrast, when the sugar adopts the C3'-endo conformation, the torsion angle about the C4'-C5' bond is in a gauche(+)-gauche- conformation. The C2'-F bond distance is 1.406(3) A, similar to that found in other aliphatic C-F bonds. The results suggest that the 2'-fluoro-2',3'-dideoxyarabinosyl nucleosides do not have a strong preference for either C2'-endo or C3'-endo sugar pucker.     

Secondary structure of the hybrid poly(rA).poly(dT) in solution. Studies involving NOE at 500 MHz and stereochemical modelling within the constraints of NOE data

One-dimensional nuclear Overhauser effect (NOE) in nuclear magnetic resonance spectroscopy along with stereochemically sound model building was employed to derive the structure of the hybrid poly(rA).poly(dT) in solution. Extremely strong NOE was observed at AH2' when AH8 was presaturated; strong NOEs were observed at TH2'TH2' when TH6 was presaturated; in addition the observed NOEs at TH2' and TH2' were nearly equal when TH6 was presaturated. There was no NOE transfer to AH3' from AH8 ruling out the possibility of (C-3'-endo, low anti chi approximately equal to 200 degrees to 220 degrees) conformation for the A residues. The observed NOE data suggest that the nucleotidyl units in both rA and dT strands have equivalent conformations: C-2'-endo/C-1'-exo, anti chi approximately equal to 240 degrees to 260 degrees. Such a nucleotide geometry for rA/dT is consistent with a right-handed B-DNA model for poly(rA).poly(dT) in solution in which the rA and dT strands are conformationally equivalent. Molecular models were generated for poly(rA).poly(dT) in the B-form based upon the geometrical constraints as obtained from the NOE data. Incorporation of (C-2'-endo pucker, chi congruent to 240 degrees to 260 degrees) into the classical B-form resulted in severe close contacts in the rA chain. By introducing base-displacement, tilt and twist along with concomitant changes in the backbone torsion angles, we were able to generate a B-form for the hybrid poly(rA).poly(dT) fully consistent with the observed NOE data. In the derived model the sugar pucker is C-1'-exo, a minor variant of C-2'-endo and the sugar base torsion is 243 degrees, the remaining torsion angles being: epsilon = 198 degrees, xi = 260 degrees, alpha = 286 degrees, beta = 161 degrees and gamma = 72 degrees; this structure is free of any steric compression and indicates that it is not necessary to switch to C-3'-endo pucker for rA residues in order to accommodate the 2'-OH group. The structure that we have proposed for the polynucleotide RNA-DNA hybrid in solution is in complete agreement with that proposed for a hexamer hybrid in solution from NOE data and is inconsistent with the heteronomous model proposed for the fibrous state.     

Solution conformation of an RNA hairpin loop.

The hairpin conformation adopted by the RNA sequence 5'GCGAUUUCUGACCGCC3' has been studied by one- and two-dimensional NMR spectroscopy. Exchangeable imino spectra in 60 mM Na+ indicate that the hairpin has a stem of six base pairs (indicated by boldface type) and a loop of three nucleotides. NOESY spectra of nonexchangeable protons confirm the formation of the stem region. The duplex has an A-conformation and contains an A.C apposition; a G.U base pair closes the loop region. The stem nucleotides have C3'-endo sugar conformations, as expected of an A-form duplex, whereas the three loop nucleotides adopt C2'-endo sugar puckers. Stacking within the loop, C8 upon the sugar of U7, stabilizes the structure. The pH dependence of both the exchangeable and nonexchangeable NMR spectra is consistent with the formation of an A+.C base pair, protonated at the N1 position of adenine. The stability of the hairpin was probed by using absorbance melting curves. The hairpin structure with the A+.C base pair is about +2 kcal/mol less stable in free energy at 37 degrees C than the hairpin formed with an A.U pair replacing the A+.C pair.     

RNA motifs that determine specificity between a viral replicase and its promoter

The 3' end of brome mosaic virus RNA contains a tRNA-like sequence that directs its RNA synthesis. A stem loop structure in this sequence, stem loop C (SLC), was investigated using NMR, and correlated with its ability to direct RNA synthesis by its replicase. SLC consists of two discrete domains, a flexible stem with an internal loop and a rigid stem containing a 5'-AUA-3' triloop. Efficient RNA synthesis requires the sequence on only one side of the flexible stem and a specific compact conformation of the triloop. A high resolution structure of the triloop places the 5' adenine out in solution, and the 3' adenine within the triloop, held tightly through stacking and unusual hydrogen bonds. This high resolution structure of an RNA promoter from a (+)-strand RNA virus provides new insights into how the RNA-dependent RNA polymerase binds to the RNA to initiate synthesis.