A phenanthrene modified RNA hairpin

The influence of hairpin loop replacement with the phenanthrene moiety in RNA was investigated. The stability of this novel structure was compared to a hairpin with a U(4) loop, an extra stable tetra-loop (UUCG), and an analogous phenanthrene modified DNA hairpin. Thermal denaturation experiments and CD spectra were used to study the structure and stability of the modified hairpin.     

Structure of 2′,5′-Linked Tetraribonucleotide Loops: A Novel RNA Motif

Abstract

We report on the three dimensional structure of an RNA hairpin containing a 2′,5′-linked tetraribonucleotide loop, namely, 5′-rGGAC(UUCG)GUCC-3′ (where UUCG = U_2′p5′U_2′p5′C_2′p5′G_2′p5′). We show that the 2′,5′-linked RNA loop adopts a conformation that is quite different from that previously observed for the native 3′,5′-linked RNA loop. The 2′,5′- RNA loop is stabilized by (a) U:G wobble base pairing, with both bases in the anti conformation, (b) extensive base stacking, and (c) sugar–base contacts, all of which contribute to the extra stability of this hairpin structure.     

Thermodynamic,structural and fluorescent characteristics of DNA hairpins containing functionalized pyrrolo-2′-deoxycytidines

Herein, we present comprehensive physicochemical and structural analysis of various DNA hairpins modified with pyrrolo-2′-deoxycytidine (Py-dC) derivatives. The introduction of modified Py-dC in most cases causes minor decrease of hairpin thermodynamic stability. The energetically unfavorable effect is more pronounced when modified residue is present within hairpin loop. Our studies indicate that thermodynamic effects induced by all Py-dC derivatives are net results of increased stacking interactions caused by larger surface of pyrrolo-2′-deoxycytidine aromatic ring and unfavorable effect implied by the presence of additional side chains. The CD spectra of all modified hairpins are similar to unmodified hairpin indicating that the presence of Py-dC derivatives does not disrupt the secondary structure of DNA. Interestingly, the presence of various side chains can increase fluorescent discrimination of paired and unpaired regions of DNA. The fluorescence observed for hairpins modified within loop is significantly quenched when Py-dC derivative is present in the stem region.     

Determination of the secondary structure of group II bulge loops using the fluorescent probe 2-aminopurine

Eleven RNA hairpins containing 2-aminopurine (2-AP) in either base-paired or single nucleotide bulge loop positions were optically melted in 1 M NaCl; and, the thermodynamic parameters ΔH°, ΔS°, ΔG°₃₇, and T_M for each hairpin were determined. Substitution of 2-AP for an A (adenosine) at a bulge position (where either the 2-AP or A is the bulge) in the stem of a hairpin, does not affect the stability of the hairpin. For group II bulge loops such as AA/U, where there is ambiguity as to which of the A residues is paired with the U, hairpins with 2-AP substituted for either the 5′ or 3′ position in the hairpin stem have similar stability. Fluorescent melts were performed to monitor the environment of the 2-AP. When the 2-AP was located distal to the hairpin loop on either the 5′ or 3′ side of the hairpin stem, the change in fluorescent intensity upon heating was indicative of an unpaired nucleotide. A database of phylogenetically determined RNA secondary structures was examined to explore the presence of naturally occurring bulge loops embedded within a hairpin stem. The distribution of bulge loops is discussed and related to the stability of hairpin structures.     

Comparison of solution conformations and stabilities of modified helix 69 rRNA analogs from bacteria and human

The helix 69 (H69) region of the large subunit (28S) ribosomal RNA (rRNA) of Homo sapiens contains five pseudouridine (Ψ) residues out of 19 total nucleotides, three of which are highly conserved. In this study, the effects of this abundant modified nucleotide on the structure and stability of H69 were compared with those of uridine in double-stranded (stem) regions. These results were compared with previous hairpin (stem plus single-stranded loop) studies to understand the contributions of the loop sequences to H69 structure and stability. The role of a loop nucleotide substitution from an A in bacteria (position 1918 in Escherichia coli 23S rRNA) to a G in eukaryotes (position 3734 in H. sapiens 28S rRNA) was examined. Thermodynamic parameters for the duplex RNAs were obtained through UV melting studies, and differences in the modified and unmodified RNA structures were examined by circular dichroism spectroscopy. The overall folded structure of human H69 appears to be similar to the bacterial RNA, consistent with the idea that ribosome structure and function are highly conserved; however, our results reveal subtle differences in structure and stability between the bacterial and human H69 RNAs in both the stem and loop regions. These findings may be significant with respect to H69 as a potential drug target site.     

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.     

Free energy of imperfect nucleic acid helices. II. Small hairpin loops

Physical studies of enzymically synthesized oligonucleotides of defined sequence are used to evaluate quantitatively the stability of small RNA hairpin loops and helices. The series (Ap)₄G(pC) _N(pU)₄, N = 4, 5 or 6, exists as monomolecular hairpin helices when N ≥ 5, and as imperfect dimer helices when N ≤ 4. In this size range, hairpin loops become more favorable (less destabilizing thermodynamically) as they increase in size from 3 to 4 to 5 unbonded nucleotides. Very small hairpin loops are particularly destabilizing; molecules whose base sequence would imply a hairpin loop of three nucleotides will generally exist with a loop of five, including a broken terminal base pair.Thermodynamic parameters for base pair and loop formation are calculated by a method which makes unnecessary the use of measured enthalpies of polynucleotide melting. Literature data on oligonucleotide double helices yield estimates of the free energy contribution from each of the six types of stacking interactions between three possible neighboring base pairs. The advantage of this approach is that the properties of oligonucleotides are used in predicting the stability of small RNA helices, avoiding the long extrapolation from the properties of high polymers.We provide Tables of temperature-dependent free energies that allow one to predict the stability and thermal transition temperature of many simple RNA secondary structures (applicable to ~1 m-Na⁺ concentration). As an example, we apply the rules to an isolated fragment of tRNA^Ser (yeast) (Coutts, 1971), whose properties were not used in calculating the free-energy parameters. The experimental melting temperature of 88 °C is predicted with an error margin of 5 deg. C.     

On loop folding in nucleic acid hairpin-type structures

In a series of studies, combining NMR, optical melting and T-jump experiments, it was found that DNA hairpins display a maximum stability when the loop part of the molecule comprises four or five nucleotide residues. This is in contrast with the current notion based on RNA hairpin studies, from which it had been established that a maximum hairpin stability is obtained for six or seven residues in the loop. Here we present a structural model to rationalize these observations. This model is based on the notion that to a major extent base stacking interactions determine the stability of nucleic acid conformations. The model predicts that loop folding in RNA is characterized by an extension of the base stacking at the 5'-side of the double helix by five or six bases; the remaining gap can then easily be closed by two nucleotides. Conversely, loop folding in DNA is characterized by extending base stacking at the 3'-side of the double helical stem by two or three residues; again bridging of the remaining gap can then be achieved by one or two nucleotides. As an example of loop folding in RNA the anticodon loop of yeast tRNAPhe is discussed. For the DNA hairpin formed by d(ATCCTAT4TAGGAT) it is shown that the loop structure obtained from molecular mechanics calculations obeys the above worded loop folding principles.     

Structure of a single-stranded DNA target as a factor influencing the effectiveness of its modification with a complementary reagent]

Site directed alkylation of three oligonucleotide targets: 41-mer (hairpin structure), 22-mer (loop part of this hairpin) and 10-mer (part of the loop) with 5'-p-(N-2-chloroethyl-N-methylamino)benzylamides of oligonucleotides complementary to the loop region was studied. Thermodynamic parameters of the interaction were estimated using the dependence of the limit modification extent on the reagent concentration at different temperatures. The stability of the complex increases much in the set: 302-mer carrying the above hairpin, 41-mer, 22-mer; data on 22-mer and 10-mer being almost identical. This indicates significant influence of the loop supporting structure on the interaction with antisense reagents.     

Tandem GA residues on opposite sides of the loop in molecular beacon-like DNA hairpins compact the loop and increase hairpin stability

The free solution electrophoretic mobilities and thermal stabilities of hairpins formed by two complementary 26-nucleotide oligomers have been measured by capillary electrophoresis. The oligomers are predicted to form molecular beacon-like hairpins with 5 bp stems and 16 nucleotides in the loop. One hairpin, called hairpin2 (hp2), migrates with a relatively fast free solution mobility and exhibits melting temperatures that are reasonably well predicted by the popular structure-prediction program Mfold. Its complement, called hairpin1 (hp1), migrates with a slower free solution mobility and forms a stable hairpin only in solutions containing ≥200 mM Na(+). The melting temperatures observed for hp1 are ~18 °C lower than those observed for hp2 and ~20 °C lower than those predicted by Mfold. The greater thermal stability of hp2 is due to the presence of tandem GA residues on opposite sides of the loop. If the corresponding TC residues in the hp1 loop are replaced by tandem GA residues, the melting temperatures of the modified hairpin are close to those observed for hp2. Eliminating the tandem GA residues in the hp2 loop significantly decreases the thermal stability of hp2. If the loops are replaced by a loop of 16 thymine residues, the free solution mobilities and thermal stabilities of the T-loop hairpin are equal to those observed for hp1. Hence, the loop of hp1 appears to be relatively unstructured, with few base-base stacking interactions. Interactions between tandem GA residues on opposite sides of the hp2 loop appear to compact the loop and increase hairpin stability.     

Preference for Ribose Over Deoxyribose in Loop-Closing Base Pairs of Extra Stable Nucleic Acid Hairpins

We have investigated the effect of switching ribose to deoxyribose at the closing base-pair of an extra-stable RNA hairpin. Specifically, we studied the sequence 5′-GGAC(UUCG)GUCC, a dodecanucleotide that folds into a well-characterized, “extra stable” RNA hairpin structure. Recently, we showed that hairpins containing a 2′,5′-linked (UUCG) loop instead of the native 3′,5′-linked loop also exhibit extra-stability (Hannoush and Damha, J. Am. Chem. Soc., 2001, 123, 12368–12374). In this article, we show that the ribose units located at the loop-closing positions (i.e., rC ₄ and rG ₉ ) contribute significantly to the stabilization of RNA hairpins, particularly those containing the 3′,5′-UUCG loop. Interestingly, the requirement of rC4 and rG9 is more relaxed for DNA hairpins containing the 2′,5′-UUCG loop and, in fact, they may be replaced altogether (ribose → deoxyribose) without affecting stability. The results broaden our understanding of the behavior of highly stable (UUCG) hairpin loops and how they respond to structural perturbation of the loop-closing base pairs.     

Non-nearest-neighbor dependence of stability for group III RNA single nucleotide bulge loops

Thirty-five RNA duplexes containing single nucleotide bulge loops were optically melted and the thermodynamic parameters for each duplex determined. The bulge loops were of the group III variety, where the bulged nucleotide is either a AG/U or CU/G, leading to ambiguity to the exact position and identity of the bulge. All possible group III bulge loops with Watson–Crick nearest-neighbors were examined. The data were used to develop a model to predict the free energy of an RNA duplex containing a group III single nucleotide bulge loop. The destabilization of the duplex by the group III bulge could be modeled so that the bulge nucleotide leads to the formation of the Watson–Crick base pair rather than the wobble base pair. The destabilization of an RNA duplex caused by the insertion of a group III bulge is primarily dependent upon non-nearest-neighbor interactions and was shown to be dependent upon the stability of second least stable stem of the duplex. In-line structure probing of group III bulge loops embedded in a hairpin indicated that the bulged nucleotide is the one positioned further from the hairpin loop irrespective of whether the resulting stem formed a Watson–Crick or wobble base pair. Fourteen RNA hairpins containing group III bulge loops, either 3′ or 5′ of the hairpin loop, were optically melted and the thermodynamic parameters determined. The model developed to predict the influence of group III bulge loops on the stability of duplex formation was extended to predict the influence of bulge loops on hairpin stability.     

The Conformation of a Conserved Stem-Loop Structure in Ribosomal RNA

Abstract

The RNA of small ribosomal subunits contains a conserved stem-loop structure near the 3′ end. Characteristics for the hairpins are: (a) a nine-basepairs stem; (b) a conserved ^A-U _U-Gjunction in the stem; (c) a conserved sequence Gm⁶ ₂Am⁶ ₂A sequence in the loop (except yeast mitochondria and mutants from bacteria). We are using UV-optics, micro-calorimetry and 500 MHz-NMR to investigate fragments of about 50 nucleotides cleaved from the 3′ ends of small ribosomal subunit RNA's by bacteriocins. Our preliminary conclusions are: (1) Dimethylation of the adenines in the loop destabilizes the hairpin because of an increased stacking; (2) melting of the hairpin starts at the ends as well as in the middle at the 5-H junction; (3) basepair substitutions have an unexpectedly large effect on thermal stability.     

Thermal stability of RNA hairpins containing a four-membered loop and a bulge nucleotide

Fourteen RNA hairpins containing a four-membered loop and a bulge nucleotide were synthesized and their thermal stabilities determined. The combined contribution of a four-membered loop and bulge A to the free energy of a hairpin is calculated to be 9.3 kcal/mol at 37 degrees C and successfully predicts the stability of an independent RNA hairpin. The introduction of a bulge nucleotide to the helical stem of an RNA hairpin destabilizes the molecule in a sequence-dependent manner. The individual thermodynamic contributions of a four-membered loop and bulge A, G, and U residues to the stability of an RNA hairpin loop are presented.     

Strong Binding of Single-stranded DNA by Stem-loop Oligonucleotides

Abstract

We report that oligodeoxynucleotides which form stem-loop hairpin structures and which have pyrimidine-rich loops can form strong complexes with complementary single-stranded DNA sequences. Stem-loop oligonucleotides were constructed with a 25-nt T-rich loop and with variable Watson-Crick stems. The complexes of these oligomers with the sequence dA_gwere studied by thermal denaturation. Evidence is presented that the complexes are one-to-one, bimolecular complexes in which the pyrimidine loop bases comprise the outer strands in a pyr · pur · pyr triplex, in effect chelating the purine strand in the center of the loop. Melting temperatures for the loop complexes are shown to be up to 29 °C higher than Watson- Crick duplex of the same length. It is shown that the presence of a stem increases stability of the triplex relative to an analogous oligomer without a stem. The effect of stem length on the stability of such a complex is examined. Such hairpin oligomers represent a new approach to the sequence-specific binding of single-stranded RNA and DNA. In addition, the finding raises the possibility that such a complex may exist in natural RNA folded sequences.     

In vitro selection of hairpin ribozymes activated with short oligonucleotides

We have carried out an in vitro selection to obtain an allosteric hairpin ribozyme, which has cleavage activity in the presence of an exogenous short oligonucleotide as a regulator. Random sequences were inserted in a region corresponding to the hairpin loop of the ribozyme. After 12 rounds of selection, DNA templates were cloned. Of a total of 34 clones, 18 contained the same sequence, and the obtained hairpin ribozymes showed the cleavage activity specifically in the presence of the regulator oligonucleotide. All of the clones contained sequences complementary to the regulator oligonucleotide. The ribozymes with high cleavage activities gained characteristic hairpin loops at the random domain, which were similar to each other. In the absence of the oligonucleotide, the loop domain within the allosteric ribozyme probably forms a slipped hairpin loop, and the complementary sequence, with the regulator oligonucleotide located at the single stranded loop, would allow easy access of the oligonucleotide. The binding of the regulator oligonucleotide triggers a structural change of the hairpin loop to form an active conformation. Furthermore, we constructed an allosteric hammerhead ribozyme by introducing the characteristic hairpin loop. The modified hammerhead ribozyme was also changed to an allosteric ribozyme, which was activated by the addition of the regulator oligonucleotide. The characteristic hairpin loop, which was proved to be regulated by an exogenous oligonucleotide in this report, may be used to control RNA functions in various fields.     

RNA hairpin loop stability depends on closing base pair.

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequences of the type GGXAUAAUAYCC, where X and Y are CG, GC, AU, UA, GU, or UG. A nearest neighbor analysis of the data indicates the free energy change for loop formation at 37 degrees C, delta degrees Gl,37, averages 3.4 kcal/mol for hairpin loops closed with C.G, G.C, and G.U pairs. In contrast, delta G degree l,37 averages 4.6 kcal/mol for loops closed with A.U, U.A, or U.G pairs. Thus the stability of an RNA hairpin depends on the closing base pair. The hairpin with a GA mismatch that is formed by GGCGUAAUAGCC is more stable than the corresponding hairpin with an AA mismatch. Thus hairpin stability also depends on loop sequence. These effects are not included in current algorithms for prediction of RNA structure from sequence.     

Coevolution of RNA helix stability and Shine-Dalgarno complementarity in a translational start region

The initiation legion of the coat-protein gene of RNA bacteriophage MS2 adopts a well-defined hairpin structure with the start codon occupying the loop position, while the Shine-Dalgarno (SD) sequence is part of the stem. In a previous study, we introduced mutations in this hairpin that changed its thermo dynamic stability. The resulting phages evolved to regain the wild-type stability by second-site compensatory substitutions. Neither the original nor the suppressor mutations were in the SD region. In the present analysis, we have made changes in the SD region that shorten or extend its complementarity to the 3 end of 16S rRNA and monitored their evolution to a stable pseudorevertant species. Phages in which the SD complementarity was decreased evolved an initiator hairpin of lower stability than wild type while those in which the complementarity was extended evolved a hairpin with an increased stability. We conclude that weaker SD sequences still allow maximal translation if the secondary structure of the ribosome-landing site is destabilized accordingly. Alternatively, translation-initiation regions with a stronger secondary structure still allow maximal expression, if the SD complementarity is extended. These findings support a previously published model in which the SD Interaction helps the ribosome to melt the structure in a translation-initiation region.