Structural characterization of three RNA hexanucleotide loops from the internal ribosome entry site of polioviruses.

Structural characteristics of three RNA hairpins from the internal ribosome entry site of poliovirus mRNAs have been determined in solution by NMR. Complete proton, phosphorus and carbon resonance assignments were made for the three 16 nt hairpins. The loop sequences, 5'-AAUCCA , AAACCA and GAACCA, have been shown to be essential for viral mRNA translation. NOESY spectra for the three oligomers were very similar indicating a common three dimensional structure. Stems were A-type duplexes with C3'-endo sugar pucker. In the loops, sequential base stacking interactions were detected for all bases except between U8/A8 and C9, indicating a turn in the phosphodiester backbone at this point. Only one nucleotide, U8/A8, had a sugar pucker which deviated appreciably from C3'-endo. The final base in the loop, A11, exhibited an unusual gauche (-) gamma angle. An ensemble of 10 structures calculated for one hairpin using restrained molecular dynamics shows that the first three bases of the loop are turned so as to be exposed to the exterior of the molecule, while the remaining three bases are in an orientation approximating a continuation of the stem helix. Structure calculations and NMR relaxation measurements indicate that the loop apex is subject to considerable local dynamics.     

The solution structure of a d[C(TTCG)G] DNA hairpin and comparison to the unusually stable RNA analogue.

The solution structure of the DNA analogue of the unusually stable r[C(UUCG)G] RNA hairpin, 5'-d[GGA-C(TTCG)GTCC]-3', has been determined by NMR spectroscopy, and its structure has been compared to that of the RNA molecule. The RNA molecule is compact and rigid with a highly structured loop. However, the DNA molecule is much less structured. The DNA hairpin contains a B-form stem of four base pairs. The terminal base pair frays, and the 3'-terminal nucleotides, C11 and C12, are in equilibrium between 2'-endo and 3'-endo conformations. Unlike the RNA loop, the DNA loop contains no syn nucleotides, and there is no evidence for base-base or base-phosphate hydrogen bonding in the loop. The loop is flexible, and reveals no specific internucleotide interactions.     

Structure of a small RNA hairpin.

The hairpin stem-loop form of the RNA oligonucleotide rCGC(UUU)GCG has been studied by NMR spectroscopy. In 10 mM phosphate buffer this RNA molecule forms a unimolecular hairpin with a stem of three base pairs and a loop of three uridines, as judged by both NMR and UV absorbance melting behavior. Distance and torsion angle restraints were determined using homonuclear proton-proton and heteronuclear proton-phosphorus 2-D NMR. These values were used in restrained molecular dynamics to determine the structure of the hairpin. The stem has characteristics of A-form geometry, although distortion from A-form occurs in the 3'-side of the stem, presumably to aid in accommodating the small loop. The loop nucleotides adopt C2'-endo conformations. NOE's strongly suggest stacking of the uracils with the stem, especially the first uracil on the 5'-side of the loop. The reversal of the chain direction in the loop seems to occur between U5 and U6. Loop structures produced by molecular dynamics simulations had a wide range of conformations and did not show stacking of the uracils. A flexible loop with significant dynamics is consistent with all the data.     

Structure of a U.U pair within a conserved ribosomal RNA hairpin.

A conserved hairpin corresponding to nt 1057-1081 of large subunit rRNA (Escherichia coli numbering) is part of a domain targeted by antibiotics and ribosomal protein L11. The stem of the hairpin contains a U.U juxtaposition, found as either U.U or U.C in virtually all rRNA sequences. This hairpin has been synthesized and most of the aromatic and sugar protons were assigned by two-dimensional proton NMR. Distances and sugar puckers deduced from the NMR data were combined with restrained molecular dynamics calculations to deduce structural features of the hairpin. The two U residues are stacked in the helix, form one NH3-O4 hydrogen bond and require an extended backbone conformation (trans alpha and gamma) at one of the U nucleotides. The hairpin loop, UAGAAGC closed by a U-A pair, is the same size as tRNA anticodon loops, but not as well ordered.     

Hairpin structures in DNA containing arabinofuranosylcytosine. A combination of nuclear magnetic resonance and molecular dynamics

Nuclear magnetic resonance (NMR) and model-building studies were carried out on the hairpin form of the octamer d(CGaCTAGCG) (aC = arabinofuranosylcytosine), referred to as the TA compound. The nonexchangeable protons of the TA compound were assigned by means of nuclear Overhauser effect spectroscopy (NOESY) and correlated spectroscopy (COSY). From a detailed analysis of the coupling data and of the NOESY spectra the following conclusions are reached: (i) The hairpin consists of a stem of three Watson-Crick type base pairs, and the two remaining residues, T(4) and dA(5), participate in a loop. (ii) All sugar rings show conformational flexibility although a strong preference for the S-type (C2'-endo) conformer is observed. (iii) The thymine does not stack upon the 3' side of the stem as expected, but swings into the minor groove. (This folding principle of the loop involves an unusual alpha t conformer in residue T(4).) (iv) At the 5'-3' loop-stem junction a stacking discontinuity occurs as a consequence of a sharp turn in that part of the backbone, caused by the unusual beta + and gamma t torsion angles in residue dG(6). (v) The A base slides over the 5' side of the stem to stack upon the aC(3) residue at the 3' side of the stem in an antiparallel fashion. On the basis of J couplings and a set of approximate proton-proton distances from NOE cross peaks, a model for the hairpin was constructed. This model was then refined by using an iterative relaxation matrix approach (IRMA) in combination with restrained molecular dynamics calculations. The resulting final model satisfactorily explains all the distance constraints.     

Use of ultra stable UNCG tetraloop hairpins to fold RNA structures: thermodynamic and spectroscopic applications.

RNA molecules of > 20 nucleotides have been the focus of numerous recent NMR structural studies. Several investigators have used the UNCG family of hairpins to ensure proper folding. We show that th UUCG hairpin has a minimum requirement of a two base-pair stem. Hairpins with a CG loop closing base pair and an initial 5'CG or 5'GC base pair have a melting temperature approximately 55 degrees C in 10 mM sodium phosphate. The high stability of even such small hairpins suggests that the hairpin can serve as a nucleation site for folding. For high resolution NMR work, the UNCG loop family (UACG in particular) provides excellent spectroscopic markers in one-dimensional exchangeable spectra, in two-dimensional COSY spectra and in NOESY spectra that clearly define it as forming a hairpin. This allows straightforward initiation of chemical shift assignments.     

DNA hairpin structures in solution: 500-MHz two-dimensional 1H NMR studies on d(CGCCGCAGC) and d(CGCCGTAGC)

A hairpin structure contains two conformationally distinct domains: a double-helical stem with Watson-Crick base pairs and a single-stranded loop that connects the two arms of the stem. By extensive 1D and 2D 500-MHz 1H NMR studies in H2O and D2O, it has been demonstrated that the DNA oligomers d(CGCCGCAGC) and d(CGCCGTAGC) form hairpin structures under conditions of low concentration, 0.5 mM in DNA strand, and low salt (20 mM NaCl, pH 7). From examination of the nuclear Overhauser effect (NOE) between base protons H8/H6 and sugar protons H1' and H2'/H2", it was concluded that in d(CGCCGCAGC) and d(CGCCGTAGC) all the nine nucleotides display average (C2'-endo,anti) geometry. The NMR data in conjunction with molecular model building and solvent accessibility studies were used to derive a working model for the hairpins.     

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.     

Proton nuclear magnetic resonance assignments and structural characterization of an intramolecular DNA triplex.

Two-dimensional 1H n.m.r. spectroscopy has been used to study the 31-base DNA oligonucleotide 5'-dAGAGAGAACCCCTTCTCTCTTTTTCTCTCTT-3', which folds to form a stable intramolecular triplex in solution at acidic pH. This structure is considerably more difficult to assign than short B-DNA duplexes and requires new assignment methods. The assignment strategy and assignments of almost all of the exchangeable and nonexchangeable resonances are presented. Seven base triplets and one Watson-Crick base-pair form the core of the structure and are connected by a four C and four T loop at either end. The second pyrimidine "strand" (bases 24 to 31) in this intramolecular pyrimidine-purine-pyrimidine triplex binds via Hoogsteen base-pairs in the major groove and is parallel to the purine "strand" (bases 1 to 8). Analysis of the sugar puckers reveals that, contrary to widely accepted belief, the triplex sugars are not predominantly in the N-type (close to C3'-endo) conformation. Except for some of the C nucleotides, all sugars are predominantly S-type (close to C2'-endo). Thus, the duplex DNA does not assume N-type sugar conformations to accommodate a third strand in the major groove. A preliminary model of the triplex structure is presented.     

Comparison of the B- and Z-form hairpin loop structures formed by d(CG)5T4(CG)5

The partially self-complementary synthetic DNA oligonucleotide d(CG)5T4(CG)5 has been studied by using 1H and 31P NMR and circular dichroism. Results show that, under low-salt conditions (120 mM NaCl buffer), an intramolecular hairpin loop exists in which the double-helical stem region is B-form and the thymidine loop residues have predominantly southern (C2'-endo) sugar conformations. The thymidine glycosidic torsion angles are intermediate between syn and anti or exist as an equilibrium mixture of residues in the two extremes. NOESY data indicate that the structure of the loop region is very similar to that found for d(CG)2T4(CG)2 [Hare, D. R., & Reid, B. R. (1986) Biochemistry 25, 5341-5350]. Under high-salt conditions (6 M NaClO4 buffer), the dominant form (approximately equal to 85%) is an intramolecular hairpin structure in which the stem region forms a Z-form double helix. As in the B-form, the loop thymidine residues are intermediate between the syn and anti conformations or exist as an equilibrium mixture of the two, but the thymidine sugar conformations differ in that they are biased toward northern (C3'-endo) conformations.     

Solution structure of the dodecamer d-(CATGGGCC-CATG)2 is B-DNA. Experimental and molecular dynamics study

The DNA duplex d-(CATGGGCCCATG)2 has been studied in solution by FTIR, NMR and CD. The experimental approaches have been complemented by series of large-scale unrestrained molecular dynamics simulation with explicit inclusion of solvent and counterions. Typical proton-proton distances extracted from the NMR spectra and the CD spectra are completely in agreement with slightly modified B-DNA. By molecular dynamics simulation, starting from A-type sugar pucker, a spontaneous repuckering to B-type sugar pucker was observed. Both experimental and theoretical approaches suggest for the dodecamer d-(CATGGGCCCATG)2 under solution conditions puckering of all 2'-deoxyribose residues in the south conformation (mostly C2'-endo) and can exclude significant population of sugars in the north conformation (C3'-endo). NMR, FTIR and CD data are in agreement with a B-form of the dodecamer in solution. Furthermore, the duplex shows a cooperative B-A transition in solution induced by addition of trifluorethanol. This contrasts a recently published crystal structure of the same oligonucleotide found as an intermediate between B- and A-DNA where 23 out of 24 sugar residues were reported to adopt the north (N-type) conformation (C3'-endo) like in A-DNA (Ng, H. L., Kopka, M. L. and Dickerson, R. E., Proc. Natl. Acad. Sci. U S A 97, 2035-2039 (2000)). The simulated structures resemble standard B-DNA. They nevertheless show a moderate shift towards A-type stacking similar to that seen in the crystal, despite the striking difference in sugar puckers between the MD and X-ray structures. This is in agreement with preceding MD reports noticing special stacking features of G-tracts exhibiting a tendency towards the A-type stacking supported by the CD spectra also reflecting the G-tract stacking. MD simulations reveal several noticeable local conformational variations, such as redistribution of helical twist and base pair roll between the central GpC steps and the adjacent G-tract segments, as well as a substantial helical twist variability in the CpA(TpG) steps combined with a large positive base pair roll. These local variations are rather different from those seen in the crystal.     

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.     

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.     

Conformation and dynamics of an RNA internal loop

The conformation and the dynamics of an RNA oligonucleotide (26 nucleotides) which is a model for loop E in eukaryotic 5S RNA have been investigated by one- and two-dimensional NMR. The central portion of the oligonucleotide contains two G A oppositions, a common feature of ribosomal RNAs. The exchangeable proton spectrum indicates that an internal loop separates two stems of four and five base pairs. This observation is not consistent with structures for loop E containing mismatched G.A base pairs proposed from chemical and enzymatic studies on Xenopus laevis 5S RNA. The nonexchangeable proton spectrum has been assigned by two-dimensional NMR. Scalar couplings from correlated experiments and interproton distances from NOESY experiments at short mixing times have been used to determine glycosidic angles, sugar puckers, and other conformational features. The conformation of the stems is very close to standard A-form RNA, and extensive base stacking continues into the internal loop. This result provides a structural basis for the large favorable enthalpy of duplex formation determined in thermodynamic studies. Unusual structural and dynamic features are localized in the nucleotides connecting the loop to the stems.     

The three-dimensional structure of a DNA hairpin in solution two-dimensional NMR studies and structural analysis of d(ATCCTATTTATAGGAT)

The hairpin formed by d(ATCCTATTTATAGGAT) was studied by means of two-dimensional NMR spectroscopy and conformational analysis. Almost all 1H resonances of the stem region could be assigned, while the 1H and 31P spectra of the loop region were interpreted completely; this includes the stereospecific assignment of the H5' and H5" resonances. The derivation of the detailed loop structure was carried out in a stepwise fashion including some improved and new methods for structure determination from NMR data. In the first step, the mononucleotide structures were examined. The conformational space available to the mononucleotide was scanned systematically by varying the glycosidic torsion angle and pseudorotational parameters. Each generated conformer was tested against the experimental J coupling constants and NOE parameters. In the following stage, the structures of dinucleotides and longer fragments were derived. Inter-residue distances between protons were calculated by means of a procedure in which the simulated NOEs, obtained via a relaxation-matrix approach, were fitted to the experimental NOEs without the introduction of a molecular model. In addition, the backbone torsion angles beta, gamma and epsilon were deduced from homocoupling and heterocoupling constants. These data served as constraints in the next step, in which the loop sequence was subjected to a multi-conformer generation procedure. The resulting structures were tested against the mentioned constraints and disregarded if these constraints were violated. This yielded a family of structures for the loop region, confined to a relatively narrow conformational space. A representative conformation was subsequently docked on a B-type stem which fulfilled the structural constraints (derived from the NMR experiments for the stem region) to yield the hairpin structure. Results obtained from subsequent restrained-molecular-mechanics as well as free-molecular-mechanics calculations are in accordance with those obtained by means of the analysis described above. The structure of the hairpin loop is a compactly folded conformation and the first base of the central TTTA region forms a Hoogsteen T-A pair with the fourth base. This Hoogsteen base pair is stacked upon the sixth base pair of the B-type double-helical stem. The second base of the loop is folded into the minor groove, whereas the third base of the loop is partly stacked on the first and fourth bases. The phosphate backbone exhibits a sharp turn between the third and fourth nucleotides of the loop. The peculiar structure of this hairpin loop is discussed in relation to loop folding in DNA and RNA hairpins and in relation to a general model for loop folding.     

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.     

Characterization of a parallel-stranded DNA hairpin

Recently we have shown that synthetic DNA containing homooligomeric A-T base pairs can form a parallel-stranded intramolecular hairpin structure [van de Sande et al. (1988) Science (Washington, D.C.) 241, 551-557]. In the present study, we have employed NMR and optical spectroscopy to investigate the structure of the parallel-stranded (PS) DNA hairpin 3'-d(T)8C4(A)8-3' and the related antiparallel (APS) hairpin 5'-d(T)8C4(A)8-3'. The parallel orientation of the strands in the PS oligonucleotide is achieved by introducing a 5'-5' phosphodiester linkage in the hairpin loop. Ultraviolet spectroscopic and fluorescence data of drug binding are consistent with the formation of PS and APS structures, respectively, in these two hairpins. Vacuum circular dichroism measurements in combination with theoretical CD calculations indicate that the PS structure forms a right-handed helix. 31P NMR measurements indicate that the conformation of the phosphodiester backbone of the PS structure is not drastically different from that of the APS control. The presence of slowly exchanging imino protons at 14 ppm and the observation of nuclear Overhauser enhancement between imino protons and the AH-2 protons demonstrate that similar base pairing and base stacking between T and A residues occur in both hairpins. However, the small chemical shift dispersion observed in proton NMR spectra of the PS hairpin suggests that the stem of this hairpin is more regular than that of the APS hairpin. On the basis of NOESY measurements, we find that the orientation of the bases is in the anti region and that the sugar puckering is in the 2'-endo range.(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformational and model-building studies of the hairpin form of the mismatched DNA octamer d(m5C-G-m5C-G-T-G-m5C-G)

The hairpin form of the mismatched octamer d(m5C-G-m5C-G-T-G-m5C-G) was studied by means of NMR spectroscopy. In a companion study it is shown that the hairpin form of this DNA fragment consists of a structure with a stem of three Watson-Crick-type base pairs and a loop consisting of only two nucleotides. The non-exchangeable proton resonances were assigned by means of two-dimensional correlation spectroscopy and two-dimensional nuclear Overhauser effect spectroscopy. Proton-proton coupling constants were used for the conformational analysis of the deoxyribose ring and for some of the backbone torsion angles. From the two-dimensional NMR spectra and the coupling-constant analysis it is concluded that: (i) the stem of the hairpin exhibits B-DNA characteristics; (ii) the sugar rings are not conformationally pure, but display a certain amount of conformational flexibility; (iii) the stacking interaction in the stem of the hairpin is elongated from the 3'-side in a more or less regular fashion with the two loop nucleotides; (iv) at the 5'-side of the stem a stacking discontinuity occurs between the stem and the loop; (v) at the 5'-side of the stem the loop is closed by means of a sharp backbone turn which involves unusual gamma' and beta+ torsion angles in residue dG(6). The NMR results led to the construction of a hairpin-loop model which was energy-minimized by means of a molecular-mechanics program. The results clearly show that a DNA hairpin-loop structure in which the loop consists of only two nucleotides bridging the minor groove in a straightforward fashion, (i) causes no undue steric strain, and (ii) involves well-known conformational principles throughout the course of the backbone. The hairpin form of the title compound is compared with the hairpin form of d(A-T-C-C-T-A-T4-T-A-G-G-A-T), in which the central -T4- part forms a loop of four nucleotides. Both models display similarities as far as stacking interactions are concerned.