A DNA hairpin with a single residue loop closed by a strongly distorted Watson-Crick G x C base-pair

Our previous NMR and modeling studies have shown that the single-stranded 19mer oligonucleotides d(AGCTTATC-ATC-GATAA GCT) -ATC- and d(AGCTTATC-GAT-GATAAGCT) -GAT- encompassing the strongest topoisomerase II cleavage site in pBR322 DNA could form stable hairpin structures. A new sheared base-pair, the pyrimidine-purine C x A, was found to close the single base -ATC- loop, while -GAT- displayed a flexible loop of three/five residues with no stabilizing interactions. Now we report a structural study on -GAC-, an analog of -GAT-, derived through the substitution of the loop residue T by C. The results obtained from NMR, non-denaturing PAGE, UV-melting, circular dichroism experiments and restrained molecular dynamics indicate that -GAC- adopts a hairpin structure folded through a single residue loop. In the -GAC- hairpin the direction of the G9 sugar is reversed relative to the C8 sugar, thus pushing the backbone of the loop into the major groove. The G9 x C11 base-pair closing the loop is thus neither a sheared base-pair nor a regular Watson-Crick one. Although G9 and C11 are paired through hydrogen bonds of Watson-Crick type, the base-pair is not planar but rather adopts a wedge-shaped geometry with the two bases stacked on top of each other in the minor groove. The distortion decreases the sugar C1'-C1' distance between the paired G9 and C11, to 8 A versus 11 A in the standard B-DNA. The A10 residue at the center of the loop interacts with the G9 x C11 base-pair, and seems to contribute to the extra thermal stability displayed by -GAC- compared to -GAT-. Test calculations allowed us to identify the experimental NOEs critical for inducing the distorted G.C Watson-Crick base-pair. The preference of -GAC- for a hairpin structure rather than a duplex is confirmed by the diffusion constant values obtained from pulse-field gradient NMR experiments. All together, the results illustrate the high degree of plasticity of single-stranded DNAs which can accommodate a variety of turn-loops to fold up on themselves.     

Solution structure of a DNA double helix incorporating four consecutive non-Watson-Crick base-pairs

A series of DNA 21-mers containing a variety of the 4 x 4 internal loop sequence 5'-CAAG-3'/3'-ACGT-5' were studied using nuclear magnetic resonance (NMR) methodology and distance geometry (DG)/molecular dynamics (MD) approaches. Such oligomers exhibit excellent resolution in the NMR spectra and reveal many unusual NOEs (nuclear Overhauser effect) that allow for the detailed characterization of a DNA hairpin incorporating a track of four different non-Watson-Crick base-pairs in the stem. These include a wobble C.A base-pair, a sheared A.C base-pair, a sheared A.G base-pair, and a wobble G.T base-pair. Significantly different twisting angles were observed between the base-pairs in internal loop that results with excellent intra-strand and inter-strand base stacking within the four consecutive mismatches and the surrounding canonical base-pairs. This explains why it melts at 52 degrees C even though five out of ten base-pairs in the stem adopt non-Watson-Crick pairs. However, the 4 x 4 internal loop still fits into a B-DNA double helix very well without significant change in the backbone torsion angles; only zeta torsion angles between the tandem sheared base-pairs are changed to a great extent from the gauche(-) domain to the trans domain to accommodate the cross-strand base stacking in the internal loop. The observation that several consecutive non-canonical base-pairs can stably co-exist with Watson-Crick base-pairs greatly increases the limited repertoire of irregular DNA folds and reveals the possibility for unusual structural formation in the functionally important genomic regions that have potential to become single-stranded.     

Analysis of melting transitions of the DNA hairpins formed from the oligomer sequences d[GGATAC(X)4GTATCC] (X = A, T, G, C)

Optical melting transitions of the short DNA hairpins formed from the self-complementary DNA oligomers d[GGATACX4GTATCC] where X = A, T, G, or C measured in 100 mM NaCl are presented. A significant dependence of the melting transitions on loop sequence is observed and transition temperatures, tm, of the hairpins vary from 58.3 degrees C for the T4 loop hairpin to 55.3 degrees C for the A4 loop. A nearest-neighbor sequence-dependent theoretical algorithm for calculating melting curves of DNA hairpins is presented and employed to analyze the experimental melting transitions. Experimental melting curves were fit by adjustment of a single theoretical parameter, Fend(n), the weighting function for a hairpin loop comprised of n single-strand bases. Empirically determined values of Fend(n) provide an evaluation of the free-energy of hairpin loop formation and stability. Effects of heterogeneous nearest-neighbor sequence interactions in the duplex stem on hairpin loop formation were investigated by evaluating Fend(n) in individual fitting procedures using two of the published sets of nearest-neighbor stacking interactions in DNA evaluated in 100 mM NaCl and given by Wartell and Benight, 1985. In all cases, evaluated values of Fend(n) were obtained that provided exact theoretical predictions of the experimental transitions. Results of the evaluations indicate: (1) Evaluated free-energies of hairpin loop formation are only slightly dependent on loop sequences examined. At the transition temperature, Tm, the free-energy of forming a loop of four bases is approximately equal for T4, G4, or C4 loops and varies from 3.9 to 4.8 kcal/mole depending on the set of nearest-neighbor interactions employed in the evaluations. This result suggests, in light of the observed differences in stability between the T4, G4, and C4 loop hairpins, that sequence-dependent interactions between base residues of the loop are most likely not the source of the enhanced stability of a T4 loop.(ABSTRACT TRUNCATED AT 400 WORDS)     

Stable sheared A.C pair in DNA hairpins

Single-residue d(Pu1NPu2) (Pu1.Pu2=G.A, G.G or A.A) hairpin loops can be stably closed by sheared purine.purine pairs. These special motifs have been found in several important biological systems. We now extend these loop-closing base-pairs to a sheared purine. pyrimidine (A.C) pair at a neutral pH condition. High-resolution NMR spectroscopy, distance geometry, and molecular dynamics methods were used to study d(GTACANCGTAC) oligomers. Numerous idiosyncratic nuclear Overhauser enhancements, especially those across the A.C base-pair between C4NH2left and right arrow AH1', C4NH2left and right arrow AH2, and CH5left and right arrow AH2 proton pairs, clearly define the novel sheared nature of the closing A.C base-pair. This novel base-pair is possibly present in several biological systems and in two single-stranded DNA aptamers selected from oligonucleotide libraries.     

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.     

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.     

Sheared-type G(anti).C(syn) base-pair: a unique d(GXC) loop closure motif

Stable DNA loop structures closed by a novel G.C base-pair have been determined for the single-residue d(GXC) loops (X=A, T, G or C) in low-salt solution by high-resolution nuclear magnetic resonance (NMR) techniques. The closing G.C base-pair in these loops is not of the canonical Watson-Crick type, but adopts instead a unique sheared-type (trans Watson-Crick/sugar-edge) pairing, like those occurring in the sheared mismatched G.A or A.C base-pair, to draw the two opposite strands together. The cytidine residue in the closing base-pair is transformed into the rare syn domain to form two H-bonds with the guanine base and to prevent the steric clash between the G 2NH(2) and the C H-5 protons. Besides, the sugar pucker of the syn cytidine is still located in the regular C2'-endo domain, unlike the C3'-endo domain adopted for the pyrimidines of the out-of-alternation left-handed Z-DNA structure. The facile formation of the compact d(GXC) loops closed by a unique sheared-type G(anti).C(syn) base-pair demonstrates the great potential of the single-stranded d(GXC) triplet repeats to fold into stable hairpins.     

Structure of a T4 hairpin loop on a Z-DNA stem and comparison with A-RNA and B-DNA loops

The synthetic DNA oligomer C-G-C-G-C-G-T-T-T-T-C-G-C-G-C-G crystallizes as a Z-DNA hexamer, capped at one end by a T4 loop. The crystals are monoclinic, space group C2, with a = 57.18 A, b = 21.63 A, c = 36.40 A, beta = 95.22 degrees, and one hairpin molecule per asymmetric unit. The structure of the z-hexamer stem was determined by molecular replacement, and the T4 loop was positioned by difference map methods. The final R factor at 2.1 A resolution for hairpin plus 70 water molecules is 20% for 2 sigma data, with a root-mean-square error of 0.26 A. The (C-G)3 stem resembles the free Z-DNA hexamer with minor crystal packing effects. The T4 loop differs from that observed on a B-DNA stem in solution, or in longer loops in tRNA, in that it shows intraloop and intermolecular interactions rather than base stacking on the final base-pair of the stem. Bases T7, T8 and T9 stack with one another and with the sugar of T7. Two T10 bases from different molecules stack between the C1-G12 terminal base-pairs of a third and fourth molecule, to simulate a T.T "base-pair". Distances between thymine N and O atoms suggest that the two thymine bases are hydrogen bonded, and a keto-enol tautomer pair is favored over disordered keto-keto wobble pairs. The hairpin molecules pack in the crystal in herringbone columns in a manner that accounts well for the observed relative crystal growth rates in a, b and c directions. Hydration seems to be most extensive around the phosphate groups, with lesser hydration within the grooves.     

Structure and function of the conserved 690 hairpin in Escherichia coli 16 S ribosomal RNA. II. NMR solution structure

The solution structure of the conserved 690 hairpin from Escherichia coli 16 S rRNA was determined by NMR spectroscopy. The 690 loop is located at the surface of the 30 S subunit in the platform region and has been implicated in interactions with P-site bound tRNA, E-site mRNA, S11 binding, IF3 binding, and in RNA-RNA interactions with the 790 loop of 16 S rRNA and domain IV of 23 S rRNA. The structure reveals a novel sheared type G690.U697 base-pair with a single hydrogen bond from the G690 amino to U697-04. G691 and A696 also form a sheared pair and U692 forms a U-turn with an H-bond to the A695 non-bridging phosphate oxygen. The sheared pairs and U-turn result in the continuous single-stranded stacking of five residues from 6693 to U697 with their Watson-Crick functional groups exposed in the minor groove. The overall fold of the 690 hairpin is similar to the anticodon loop of tRNA. The structure provides an explanation for chemical protection patterns in the loop upon interaction with tRNA, the 50 S subunit, and S11. In vivo genetic studies demonstrate the functional importance of the motifs observed in the solution structure of the 690 hairpin.     

The B-Z conformational transition in folded oligodeoxynucleotides: loop size and stability of Z-hairpins

The capacity to assume a left-handed conformation and the thermodynamics of loop formation in concentrated aqueous NaClO4 have been investigated for the following palindromic sequences: d-(CGCGCGAAAAACGCGCG) (A5), d(CGCGCGTTTTTCGCGCG) (T5), d(CGCGCGTACGCGCG) (TA), and d(CGCGCGATCGCGCG) (AT). The results show that (a) each oligomer assumes a Z conformation upon exposure to increasing NaClO4 concentrations; the salt concentration at the transition midpoint is 1.8 M for both A5 and T5 and 3 and 3.5 M for TA and AT, respectively; (b) in high salt the four oligomers exist, over a wide range of nucleotide concentrations (up to 10(-3) M) and of temperature (greater than 0 degrees C), as unimolecular hairpin structures; (c) hairpins TA and AT exhibit, in buffer A, a lower thermal stability with respect to A5 and T5 (delta T about 16 degrees C), contrary to what is observed at low ionic strength; (d) on hairpin formation, the enthalpic term is about -52 kcal/mol for the two 17-mers and -38 kcal/mol for the two 14-mers, while the change in entropy is found to be around -150 eu for A5 and T5 and -115 eu for TA and AT. This thermodynamic picture suggests that a two-residue loop for TA and AT, found at low ionic strength [see preceding paper (Xodo, L.E., Manzini, G., Quadrifoglio, F., van der Marel, G.A., & van Boom, J.H. (1988) Biochemistry (preceding paper in this issue)], is substituted by a longer one including two additional residues from a missing dC.dG base pairing at the top of the stem.     

Oligodeoxynucleotide folding in solution: loop size and stability of B-hairpins

The secondary structures of the synthetic DNA fragments d(CGCGCGTTTTTCGCGCG) (T5), d(CGCGCGAAAAACGCGCG) (A5), d(CGCGCGTACGCGCG) (TA), and d(CGCGCGATCGCGCG) (AT) were investigated in a combined electrophoretic and spectroscopic study. All the oligomers exist, at low temperature and over a wide range of ionic strength (0.5-100 mM salt) and of nucleotide concentration [0.1-2.0 mM (phosphate)], as a mixture of two slowly interconverting species, identified as the dimeric duplex and the monomeric hairpin structure. The thermodynamic parameters for hairpin denaturation of T5, A5, TA, and AT and for duplex denaturation of d(CGCGCG) show that (a) the hairpins are more stable than the reference hexamer duplex at all accessible nucleotide concentrations; (b) the loop contributes favorably to the enthalpy change of hairpin denaturation in the four DNA fragments; (c) the base composition of the loop (A vs T) and the size of the loop (A5/T5 vs TA/AT) do not appreciably influence the enthalpic contents of the hairpins; (d) hairpins TA and AT, with two AT bases intervening in the CG self-complementary part of the molecule, exhibit a markedly higher thermal stability than hairpins T5 and A5, which is entropic in origin. These findings are consistent with the presence of two-residue loops in the tetradecamers TA and AT.     

Thermodynamics of DNA hairpins: contribution of loop size to hairpin stability and ethidium binding.

A combination of calorimetric and spectroscopic techniques was used to evaluate the thermodynamic behavior of a set of DNA hairpins with the sequence d(GCGCTnGCGC), where n = 3, 5 and 7, and the interaction of each hairpin with ethidium. All three hairpins melt in two-state monomolecular transitions, with tm's ranging from 79.1 degrees C (T3) to 57.5 degrees C (T7), and transition enthalpies of approximately 38.5 kcal mol-1. Standard thermodynamic profiles at 20 degrees C reveal that the lower stability of the T5 and T7 hairpins corresponds to a delta G degree term of +0.5 kcal mol-1 per thymine residue, due to the entropic ordering of the thymine loops and uptake of counterions. Deconvolution of the ethidium-hairpin calorimetric titration curves indicate two sets of binding sites that correspond to one ligand in the stem with binding affinity, Kb, of approximately 1.8 x 10(6) M-1, and two ligands in the loops with Kb of approximately 4.3 x 10(4) M-1. However, the binding enthalpy, delta Hb, ranges from -8.6 (T3) to -11.6 kcal mol-1 (T7) for the stem site, and -6.6 (T3) to -12.7 kcal mol-1 (T7) for the loop site. Relative to the T3 hairpin, we obtained an overall thermodynamic contribution (per dT residue) of delta delta Hb = delta(T delta Sb) = -0.7(5) kcal mol-1 for the stem sites and delta delta Hb = delta(T delta Sb) = -1.5 kcal mol-1 for the loop sites. Therefore, the induced structural perturbations of ethidium binding results in a differential compensation of favorable stacking interactions with the unfavorable ordering of the ligands.     

Unusual DNA duplex and hairpin motifs

Single-stranded DNA or double-stranded DNA has the potential to adopt a wide variety of unusual duplex and hairpin motifs in the presence (trans) or absence (cis) of ligands. Several principles for the formation of those unusual structures have been established through the observation of a number of recurring structural motifs associated with different sequences. These include: (i) internal loops of consecutive mismatches can occur in a B-DNA duplex when sheared base pairs are adjacent to each other to confer extensive cross- and intra-strand base stacking; (ii) interdigitated (zipper-like) duplex structures form instead when sheared G·A base pairs are separated by one or two pairs of purine·purine mismatches; (iii) stacking is not restricted to base, deoxyribose also exhibits the potential to do so; (iv) canonical G·C or A·T base pairs are flexible enough to exhibit considerable changes from the regular H-bonded conformation. The paired bases become stacked when bracketed by sheared G·A base pairs, or become extruded out and perpendicular to their neighboring bases in the presence of interacting drugs; (v) the purine-rich and pyrimidine-rich loop structures are notably different in nature. The purine-rich loops form compact triloop structures closed by a sheared G·A, A·A, A·C or sheared-like G_anti·C_syn base pair that is stacked by a single residue. On the other hand, the pyrimidine-rich loops with a thymidine in the first position exhibit no base pairing but are characterized by the folding of the thymidine residue into the minor groove to form a compact loop structure. Identification of such diverse duplex or hairpin motifs greatly enlarges the repertoire for unusual DNA structural formation.     

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)     

Thermodynamic parameters for loop formation in RNA and DNA hairpin tetraloops.

We determined the melting temperatures (Tm) and thermodynamic parameters of 15 RNA and 19 DNA hairpins at 1 M NaCl, 0.01 M sodium phosphate, 0.1 mM EDTA, at pH 7. All these hairpins have loops of four bases, the most common loop size in 16S and 23S ribosomal RNAs. The RNA hairpins varied in loop sequence, loop-closing base pair (A.U, C.G, or G.C), base sequence of the stem, and stem size (four or five base pairs). The DNA hairpins varied in loop sequence, loop-closing base pair (C.G, or G.C), and base sequence of the four base-pair stem. Thermodynamic properties of a hairpin may be represented by nearest-neighbor interactions of the stem plus contributions from the loop. Thus, we obtained thermodynamic parameters for the formation of RNA and DNA tetraloops. For the tetraloops we studied, a free energy of loop formation (at 37 degrees C) of about +3 kcal/mol is most common for either RNA or DNA. There are extra stable loops with delta G degrees 37 near +1 kcal/mol, but the sequences are not necessarily the same for RNA and DNA. The closing base pair is also important; changing from C.G to G.C lowered the stability of several tetraloops in both RNA and DNA. These values will be useful in predicting RNA and DNA secondary structures.     

Selective abstraction of 2H from C-1' of the C residue in AGC.ICT by the radical center at C-2 of activated neocarzinostatin chromophore: structure of the drug/DNA complex responsible for bistranded lesion formation.

Glutathione-activated neocarzinostatin chromophore (NCS-Chrom) generates bistranded lesions at AGC.GCT sequences in DNA, consisting of an abasic site at the C residue and a strand break at the T residue on the complementary strand, due to hydrogen atom abstraction from C-1' and C-5', respectively. Earlier work showed that 2H from C-5' of T was selectively abstracted by the radical center at C-6 of activated NCS-Chrom, supporting a proposed model of the active-drug/DNA complex. However, since under the conditions used breaks at the T exceeded their inclusion in bistranded lesions, it was not clear what fraction of the hydrogen transfer represented bistranded lesions. Since virtually all abasic sites at the C are part of a bistranded lesions, hydrogen transfer from C-1' of C into the drug should reflect only the bistranded reaction. Accordingly, a self-complementary oligodeoxynucleotide 5'-GCAGCICTGC-3' was synthesized in which the C contained 2H at the C-1' position. In order to eliminate an 2H isotope effect on the transfer and to increase the extent of the bistranded reaction, an I residue was substituted for the G opposite the C residue. Sequencing gel electrophoretic analysis revealed that under one-hit kinetics, 37% of the damage reaction was associated with abasic site (alkali-labile break) formation at the C residue and 48% with direct strand breaks at the T residue. Thus, 74% of the damage involved a bistranded lesion. 1H NMR spectroscopic analysis of the reacted chromophore showed that 2H had been selectively transferred into the C-2 position to the extent of approximately 22%.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Rigid spin-labeled nucleoside C: a nonperturbing EPR probe of nucleic acid conformation

Rigid spin-labeled nucleoside C, an analog of deoxycytidine that base-pairs with deoxyguanosine, was incorporated into DNA oligomers by chemical synthesis. Thermal denaturation experiments and circular dichroism (CD) measurements showed that C has a negligible effect on DNA duplex stability and conformation. Nucleoside C was incorporated into several positions within single-stranded DNA oligomers that can adopt two hairpin conformations of similar energy, each of which contains a four-base loop. The relative mobility of nucleotides in the alternating C/G hairpin loops, 5'-d(GCGC) and 5'-d(CGCG), was determined by electron paramagnetic resonance (EPR) spectroscopy. The most mobile nucleotide in the loop is the second one from the 5'-end, followed by the third, first and fourth nucleotides, consistent with previous NMR studies of DNA hairpin loops of different sequences. The EPR hairpin data were also corroborated by fluorescence spectroscopy using oligomers containing reduced C (C(f)), which is fluorescent. Furthermore, EPR spectra of duplex DNAs that contained C at the end of the helix showed features that indicated dipolar coupling between two spins. These data are consistent with end-to-end duplex stacking in solution, which was only observed when G was paired to C, but not when C was paired with A, C or T.     

Targeting degradation of RNA by RNase H using DNA hairpins

RNase H degradation of two 15 nt RNA target sites was examined in the presence of hairpin DNAs with a 5 nt loop and a 10 bp stem or single-stranded 15 nt DNAs. One target site was a segment of a 79 nt RNA, and the other was part of a 53 nt RNA. Secondary structure predictions indicate that the 53 nt RNA target site is entirely single stranded, while a portion of the 79 nt RNA target site forms an intramolecular duplex. Less RNase H and DNA were needed to cleave the 53 nt RNA target site than the less accessible 79 nt RNA site. The hairpin DNAs had their 5 nt loop and 3' side of the stem fully complementary to the target sites or had sequence changes that produced one to nine mismatched pairs. T(m) values ranged from 57 to 80 degrees C. The stability of the hairpin DNAs relative to the stability of their corresponding RNA-DNA hybrids influenced the extent of RNase H degradation at 37 degrees C. Under the assay conditions employed, the amount of degradation directed by the hairpin DNAs was correlated with their predicted DeltaG(o) (37) of binding to the RNA targets. A DNA hairpin with one mismatch to the target site of the 79 nt RNA did not induce degradation under conditions where fully complementary DNA hairpins produced 50-80% degradation. The in vitro results indicate that DNA hairpins can enhance the stringency of RNase H targeted degradation of the RNA sites.