NMR studies on DNA hairpin structures with a five nucleotide loop

One- and two-dimensional NMR experiments have been undertaken to investigate the structure of DNA hairpins with a five nucleotide loop. Analysis of proton NMR spectra suggests that the four hairpin structures examined have some common structural features; B-type conformation in the stem region and the same stacking pattern, 5' (XXX-turn-XX) 3', in the loop region. The phosphorus NMR spectra suggest that the conformational changes in the loop region affect the backbone conformation of the stem duplex.     

Multinuclear NMR studies of DNA hairpins. 2. Sequence-dependent structural variations

The solution conformation of three related DNA hairpins, each with five bases in the loop, is investigated by proton and phosphorus 2D NMR methods. The sequences of the three oligomers are d(CGCGTTGTTCGCG), d(CGCGTTTGTCGCG), and d(CTGCTCTTGTTGAGCAG). One pair of hairpins shares the same stem sequence but differs in the loop, and the appearance of an unusual phosphate torsion in the stem is found to depend on the sequence in the loop of the hairpin. The second pair of hairpins shares the same loop region but differs in the stem sequence in that the base pair which closes the loop is a C-G or G-C pair. The pattern of NOEs reveals that the stacking arrangement in the loop region depends on the base pair that closes the stem. These results suggest that hairpin loop conformation and dynamics are sensitive to small changes in the loop and adjacent stem sequences. These findings are discussed in relation to sequence-dependent thermodynamic changes that have been observed in RNA hairpins.     

Multinuclear NMR studies of DNA hairpins. 1. Structure and dynamics of d(CGCGTTGTTCGCG)

The solution structure of the hairpin formed by d(CGCGTTGTTCGCG) has been examined in detail by a wide variety of NMR techniques. The hairpin was characterized by proton NMR to obtain interproton distances and torsion angle information. An energy-minimized model was constructed that is consistent with these data. The hairpin consists of a B-DNA stem of four C-G base pairs and a loop region consisting of five unpaired bases. Three bases in the 5' of the loop are stacked over the 3' end of the stem, and the other two bases in the 3' of the loop are stacked over the 5' end of the stem. The phosphorus NMR spectrum revealed a phosphate in the stem region with an unusual conformation, and two phosphates, P9 and P10, were found to undergo intermediate exchange between conformations. The hairpin was also synthesized with a carbon-13 label in each of the thymidine C6 carbons, and relaxation measurements were performed to determine the extent of internal motions in the loop region. The loop bases are more flexible than the stem bases and exhibit subnanosecond motions with an amplitude corresponding to diffusion in a cone of approximately 30 degrees.     

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.     

Perturbation of DNA hairpins containing the EcoRI recognition site by hairpin loops of varying size and composition: physical (NMR and UV) and enzymatic (EcoRI) studies.

We have investigated loop-induced structural perturbation of the stem structure in hairpins d(GAATTCXnGAATTC) (X = A, T and n = 3, 4, 5 and 6) that contain an EcoRI restriction site in close proximity to the hairpin loop. Oligonucleotides containing either a T3 or a A3 loop were not hydrolyzed by the restriction enzyme and also showed only weak binding to EcoRI in the absence of the cofactor Mg2+. In contrast, hairpins with larger loops are hydrolyzed by the enzyme at the scission site next to the loop although the substrate with a A4 loop is significantly more resistant than the oligonucleotide containing a T4 loop. The hairpin structures with 3 loop residues were found to be thermally most stable while larger hairpin loops resulted in structures with lower melting temperatures. The T-loop hairpins are thermally more stable than the hairpins containing the same number of A residues in the loop. As judged from proton NMR spectroscopy and the thermodynamic data, the base pair closest to the hairpin loop did form in all cases studied. The hairpin loops did, however, affect the conformation of the stem structure of the hairpins. From 31P and 1H NMR spectroscopy we conclude that the perturbation of the stem structure is stronger for smaller hairpin loops and that the extent of the perturbation is limited to 2-3 base pairs for hairpins with T3 or A4 loops. Our results demonstrate that hairpin loops modulate the conformation of the stem residues close to the loop and that this in turn reduces the substrate activity for DNA sequence specific proteins.     

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.     

Structural characterization of a six-nucleotide RNA hairpin loop found in Escherichia coli, r(UUAAGU)

The binding region of the Escherichia coli S2 ribosomal protein contains a conserved UUAAGU hairpin loop. The structure of the hairpin formed by the oligomer r(GCGU4U5A6A7G8U9CGCA), which has an r(UUAAGU) hairpin loop, was determined by NMR and molecular modeling techniques as part of a study aimed at characterizing the structure and thermodynamics of RNA hairpin loops. Thermodynamic data obtained from melting curves for this RNA oligomer show that it forms a hairpin in solution with the following parameters: DeltaH degrees = -42.8 +/- 2.2 kcal/mol, DeltaS degrees = -127.6 +/- 6.5 eu, and DeltaG degrees (37) = -3.3 +/- 0.2 kcal/mol. Two-dimensional NOESY WATERGATE spectra show an NOE between U imino protons, which suggests that U4 and U9 form a hydrogen bonded U.U pair. The U5(H2') proton shows NOEs to both the A6(H8) proton and the A7(H8) proton, which is consistent with formation of a "U" turn between nucleotides U5 and A6. An NOE between the A7(H2) proton and the U9(H4') proton shows the proximity of the A7 base to the U9 sugar, which is consistent with the structure determined for the six-nucleotide loop. In addition to having a hydrogen-bonded U.U pair as the first mismatch and a U turn, the r(UUAAGU) loop has the G8 base protruding into the solvent. The solution structure of the r(UUAAGU) loop is essentially identical to the structure of an identical loop found in the crystal structure of the 30S ribosomal subunit where the guanine in the loop is involved in tertiary interactions with RNA bases from adjacent regions [Wimberly, B. T., Brodersen, D. E., Clemons, W. M., Morgan-Warren, R. J., Carter, A. P., Vonrhein, C., Hartsch, T., and Ramakrishnan, V. (2000) Nature 407, 327-339]. The similarity of the solution and solid-state structures of this hairpin loop suggests that formation of this hairpin may facilitate folding of 16S RNA.     

The structure of the L3 loop from the hepatitis delta virus ribozyme: a syn cytidine.

The structure of the L3 central hairpin loop isolated from the antigenomic sequence of the hepatitis delta virus ribozyme with the P2 and P3 stems from the ribozyme stacked on top of the loop has been determined by NMR spectroscopy. The 26 nt stem-loop structure contains nine base pairs and a 7 nt loop (5'-UCCUCGC-3'). This hairpin loop is critical for efficient catalysis in the intact ribozyme. The structure was determined using homonuclear and heteronuclear NMR techniques on non-labeled and15N-labeled RNA oligonucleotides. The overall root mean square deviation for the structure was 1.15 A (+/- 0.28 A) for the loop and the closing C.G base pair and 0.90 A (+/- 0.18 A) for the loop and the closing C.G base pair but without the lone purine in the loop, which is not well defined in the structure. The structure indicates a U.C base pair between the nucleotides on the 5'- and 3'-ends of the loop. This base pair is formed with a single hydrogen bond involving the cytosine exocyclic amino proton and the carbonyl O4 of the uracil. The most unexpected finding in the loop is a syn cytidine. While not unprecedented, syn pyrimidines are highly unusual. This one can be confidently established by intranucleotide distances between the ribose and the base determined by NMR spectroscopy. A similar study of the structure of this loop showed a somewhat different three-dimensional structure. A discussion of differences in the two structures, as well as possible sites of interaction with the cleavage site, will be presented.     

The Hairpin Structure of a Topoisomerase II Site DNA Strand Analyzed by Combined NMR and Energy Minimization Methods

We report on the structural study of the single-stranded 19mer oligonucleotide d(AGCTTATC-ATC-GATAAGCT) 22(+). This corre sponds to the 15-to-33(+) strand of pBR322 DNA belonging to a strong cleavage site (site 22) for topoisomerase II coupled to antitumor drugs VP-16 or ellipticine. The partially self-complementary nature of this oligonucleotide makes likely its folding into a hairpin structure. To assess this property we carried out a quantitative analysis based on joint calculations and NMR experiments. The latter required two-dimensional (NOESY, P-COSY, TOCSY and proton-detected¹H-³¹P), and three- dimensional (NOESY-TOCSY) spectra to achieve the assignment of the overcrowded sugar H4′ ad H5′/H5′′ proton region. For molecular modeling, the JUMNA program was used together with NMR constraints; namely, the distances and the backbone torsion angles provided by NOEs and homo- and heteronuclear coupling constants. Experimental results proved that the 19mer oligonucleotide adopted a stable hairpin structure characterized by an eight base-pair stem and a three-membered loop (central-ATC-segment). Homonuclear¹H-¹H and heteronuclear¹H-³¹P coupling constant measurements provided information on the confor mational heterogeneity of the sugar and phosphate groups within both the stem and the loop. Restrained energy minimizations starting with different structures resulted in a family of closely related structures. All low-energy molecules presented the same, rather compact, folded structure with the base-stacking continuing into the loop, a sharp turn occurring between residues T10 and C11, and strong backbone distortions at the loop-stem junction.     

Protonation of deoxycytidine residues in dC4 tetraloops: UV spectrophotometric study of dC10 and d(A14C4T14)

It is shown that component analysis could be applied to study the UV difference spectra of cytidine oligomers and hairpin oligonucleotides with cytidines in the loop region in order to account for the melting and titration results in terms of cytidine stacking and protonation. Upon acid titration, the dC(10) oligomer undergoes cooperative conformational transition at pH 6.3 accompanied by protonation and formation of the i-structure with half of the residues protonated. The stability of the hemiprotonated structure increases with decreasing pH, the i-structure persisting still in the region of pH相似文献   

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.     

Hairpin and duplex formation in DNA fragments CCAATTTTGG, CCAATTTTTTGG, and CCATTTTTGG: a proton NMR study

Three DNA fragments, CCAATTTTGG (1), CCAATTTTTTGG (2), and CCATTTTTGG (3), were studied by proton NMR spectroscopy in aqueous solution. All these oligodeoxyribonucleotides contain common sequences at the 5' and 3' ends (5'-CCA and TGG-3'). 2 as well as 3 forms only hairpin structures with four unpaired thymidylyl units, four and three base pair stems, respectively, in neutral solution under low and high NaCl concentrations. At high salt concentration the oligomer 1 forms a duplex structure with -TT- internal loop. On the other hand, the same oligomer forms a stable hairpin structure at low salt and low strand concentrations at pH 7. The hairpin structure of 1 has a stem containing only three base pairs (CCA.TGG) and a loop containing four nucleotides (-ATTT-) that includes a dissociated A.T base pair. The two secondary structures of 1 coexist in an aqueous solution containing 0.1 M NaCl, at pH 7. The equilibrium shifts to the hairpin side when the temperature is raised. The stabilities and base-stacking modes of all three oligonucleotides in two different structures are reported.     

Structure and dynamics of the DNA hairpins formed by tandemly repeated CTG triplets associated with myotonic dystrophy.

Anomalous expansion of the DNA triplet (CTG)n causes myotonic dystrophy. Structural studies have been carried out on (CTG)n repeats in an attempt to better understand the molecular mechanism of repeat expansion. NMR and gel electrophoretic studies demonstrate the presence of hairpin structures for (CTG)5 and (CTG)6 in solution. The monomeric hairpin structure remains invariant over a wide range of salt concentrations (10-200 mM NaCl), DNA concentrations (micromolar to millimolar in DNA strand) and pH (6.0-7.5). The (CTG)n hairpin contains three bases in the loop when n is odd and four bases when n is even. For both odd and even n the stacking and pairing in the stem remain the same, i.e, two hydrogen bond T.T pairs stack with the neighboring G.C pairs. All the nucleotides in (CTG)5 and (CTG)6 adopt C2'-endo, anti conformations. Full-relaxation matrix analysis has been performed to derive the NOE distance constraints from NOESY experiments at seven different mixing times (25, 50, 75, 100, 125, 200 and 500 ms). NOESY-derived distance constraints were subsequently used in restrained molecular dynamics simulations to obtain a family of structures consistent with the NMR data. The theoretical order parameters are computed for H5-H6(cytosines) and H2'-H2" dipolar correlations for both (CTG)5 and (CTG)6 by employing the Lipari-Szabo formalism. Experimental data show that the cytosine in the loop of the (CTG)5 hairpin is slightly more flexible than those in the stem. The cytosine in the loop of the (CTG)6 hairpin is extremely flexible, implying that the dynamics of the four base loop is intrinsically different from that of the three base loop.     

Hairpins in a DNA site for topoisomerase II studied by 1H- and 31P-NMR.

1H- and 31P-NMR and UV-absorption studies were carried out with the oligonucleotide strands d(AGCT-TATC-ATC-GATAAGCT) (-ATC-) and d(AGCTTATC-GAT-GATAAGCT) (-GAT-) contained in the strongest and salt resistant cleavage site for topoisomerase II in pBR322 DNA. We found that the two oligonucleotides were stabilized under a hairpin structure characterized by a eight base pair stem and a three base loop at low DNA and salt concentrations. In such experimental conditions, only the -GAT- oligonucleotide displayed a partial homoduplex structure in slow equilibrium with its folded structure. Temperature dependencies of imino protons showed that the partial homoduplex of -GAT- melted at a lower temperature than the hairpin structure. It was suggested that the appearance of the partial homoduplex in -GAT- is related to the formation of two stabilizing (G.T) mismatched base pairs in the central loop of this structure. Finally, it was inferred from the dispersion of chemical shifts in the 31P-NMR spectra that the distortions affecting the backbone of the hairpin loop are larger in the case of -ATC- compared with -GAT-. At the same time NOEs proved that the base stacking was stronger within the loop of the -ATC- hairpin.     

A local, interactive network of 3' RNA elements supports translation and replication of Turnip crinkle virus

The majority of the 3' untranslated region (UTR) of Turnip crinkle virus (TCV) was previously identified as forming a highly interactive structure with a ribosome-binding tRNA-shaped structure (TSS) acting as a scaffold and undergoing a widespread conformational shift upon binding to RNA-dependent RNA polymerase (RdRp). Tertiary interactions in the region were explored by identifying two highly detrimental mutations within and adjacent to a hairpin H4 upstream of the TSS that reduce translation in vivo and cause identical structural changes in the loop of the 3' terminal hairpin Pr. Second-site changes that compensate for defects in translation/accumulation and reverse the structural differences in the Pr loop were found in the Pr stem, as well as in a specific stem within the TSS and within the capsid protein (CP) coding region, suggesting that the second-site changes were correcting a conformational defect and not restoring specific base pairing. The RdRp-mediated conformational shift extended upstream through this CP open reading frame (ORF) region after bypassing much of an intervening, largely unstructured region, supporting a connection between 3' elements and coding region elements. These data suggest that the Pr loop, TSS, and H4 are central elements in the regulation of translation and replication in TCV and allow for development of an RNA interactome that maps the higher-order structure of a postulated RNA domain within the 3' region of a plus-strand RNA virus.     

The NMR structure of an internal loop from 23S ribosomal RNA differs from its structure in crystals of 50s ribosomal subunits

Internal loops play an important role in structure and folding of RNA and in recognition of RNA by other molecules such as proteins and ligands. An understanding of internal loops with propensities to form a particular structure will help predict RNA structure, recognition, and function. The structures of internal loops 5' 1009CUAAG1013 3'/3' 1168GAAGC1164 5' and 5' 998CUAAG1002 3'/3' 1157GAAGC1153 5' from helix 40 of the large subunit rRNA in Deinococcus radiodurans and Escherichia coli, respectively, are phylogenetically conserved, suggesting functional relevance. The energetics and NMR solution structure of the loop were determined in the duplex 5' 1GGCUAAGAC9 3'/3' 18CCGAAGCUG10 5'. The internal loop forms a different structure in solution and in the crystal structures of the ribosomal subunits. In particular, the crystal structures have a bulged out adenine at the equivalent of position A15 and a reverse Hoogsteen UA pair (trans Watson-Crick/Hoogsteen UA) at the equivalent of U4 and A14, whereas the solution structure has a single hydrogen bond UA pair (cis Watson-Crick/sugar edge A15U4) between U4 and A15 and a sheared AA pair (trans Hoogsteen/sugar edge A14A5) between A5 and A14. There is cross-strand stacking between A6 and A14 (A6/A14/A15 stacking pattern) in the NMR structure. All three structures have a sheared GA pair (trans Hoogsteen/sugar edge A6G13) at the equivalent of A6 and G13. The internal loop has contacts with ribosomal protein L20 and other parts of the RNA in the crystal structures. These contacts presumably provide the free energy to rearrange the base pairing in the loop. Evidently, molecular recognition of this internal loop involves induced fit binding, which could confer several advantages. The predicted thermodynamic stability of the loop agrees with the experimental value, even though the thermodynamic model assumes a Watson-Crick UA pair.     

Conformational feasibility of a hairpin with two purines in the loop. 5'-d-GGTACIAGTACC-3'

Structural feasibility and conformational requirements for the sequence 5'-d-GGTACIAGTACC-3' to adopt a hairpin loop with I6 and A7 in the loop are studied. It is shown that a hairpin loop containing only two nucleotides can readily be formed without any unusual torsional angles. Stacking is continued on the 5'-side of the loop, with the I6 stacked upon C5. The base A7, on the 3'-side of the loop, can either be partially stacked with I6 or stick outside without stacking. Loop closure can be achieved for both syn and anti conformations of the glycosidic torsions for G8 while maintaining the normal Watson-Crick base pairing with the opposite C5. All torsional angles in the stem fall within the standard B-family of DNA helical structures. The phosphodiesters of the loop have trans,trans conformations. Loop formation might require the torsion about the C4'-C5' bond of G8 to be trans as opposed to the gauche+ observed in B-DNA. These results are discussed in relation to melting temperature studies [Howard et al. (1991) Biochemistry (preceding paper in this issue)] that suggest the formation of very stable hairpin structures for this sequence.     

Novel Hoogsteen-like bases for configurational recognition of the T-A base pair by DNA triplex formation

Effective sequence-specific recognition of duplex DNA is possible by triplex formation with natural oligonucleotides via Hoogsteen H-bonding. However, triplex formation is in practice limited to pyrimidine oligonucleotides binding duplex A-T or G-C base-pair DNA sequences specifically at homopurine sites in the major groove as T·A-T and C⁺·G-C triplets. Here we report the successful modeling of novel unnatural nucleosides that recognize the T-A DNA base pair by Hoogsteen interaction. Since the DNA triplex can be considered to assume an A-type or B-type conformation, these novel Hoogsteen nucleotides are tested within model A-type and B-type conformation triplex structures. A triplet consisting of the T-A base pair and one of the novel Hoogsteen nucleotides replaces the central T·A-T triplet in the triplex using the same deoxyribose-phosphodiester and base-deoxyribose dihedral angle configuration. The entire triplex is energy minimized and the presence of any structural or energetic perturbations due to the central triplet is assessed with respect to the unmodified energy-minimized (T·A-T)₁₁ proposed starting structures. Incorporation of these novel triplets into both A-type and B-type natural triplex structures provokes minimal change in the configuration of the central and adjacent triplets. The plan is to produce a series of Hoogsteen-like bases that preferentially bind the T-A major groove in either an A-type or B-type conformation. Selective recognition of the T-A major groove with respect to the G-C major groove, which presents similar keto and amine placement, is also assessed with configurational preference. Evaluation of the triplex solution structure by using these unnatural bases as binding conformational probes is a prerequisite to the further design of triplet forming bases. © 1996 John Wiley & Sons, Inc.     

Effects of base sequence on the loop folding in DNA hairpins

High-resolution NMR and UV-melting experiments have been used to study the hairpin formation of partly self-complementary DNA fragments in an attempt to derive rules that describe the folding in these molecules. Earlier experiments on the hexadecanucleotide d(ATCCTA-TTTT-TAGGAT) had indicated that within the loop of four thymidines a wobble T-T pair is formed (Blommers et al., 1987). In the present paper it is shown that if the first and the last thymines of the intervening sequence are replaced by complementary bases, sometimes base pairs can be formed. Thus for the intervening sequences -CTTG- and -TTTA- with the pyrimidine in the 5'-position and the purine in the 3'-position, a base pair is formed leading to a loop consisting of two residues. For the intervening sequences -GTTC- and -ATTT- with the purine in the 5'-position and the pyrimidine in the 3'-position, this turns out not to be the case. It was found that it made no difference when the four-membered sequence was closed by a G-C base pair or an A-T base pair. Replacement of the two central thymidine residues by the more bulky adenine residues limits the hairpin to a four-membered loop scheme. Very surprisingly, it was found from 2D NOE experiments that the T-A base pair, formed in the loop consisting of the -TTTA- sequence, is a Hoogsteen pair. It is argued that the pairing of the bases in this scheme may facilitate the formation of a loop of two residues, since the distance of the C1' atoms in this base pair is 8.6 A instead of 10.4 A found in the canonical Watson-Crick base pair. Combination of the data obtained for the series of DNA fragments studied shows that the results can be explained by a simple, earlier proposed, loop folding principle which assumes that the folding of the four-membered loop is dictated by the stacking of the double-helical stem of the hairpin.