Conformational and Model-Building Studies of the Hairpin Form of the Mismatched DNA Octamer d(m5C-G-m5C-G-T-G-m5C-G)

Abstract

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 γ^t and β⁺ 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.     

Studies of DNA dumbbells. VI. Analysis of optical melting curves of dumbbells with a sixteen-base pair duplex stem and end-loops of variable size and sequence

Optical melting curves of 22 DNA dumbbells with the 16-base pair duplex sequence 5′-G-C-A-T-C-A-T-C-G-A-T-G-A-T-G-C-3′ linked on both ends by single-strand loops of A_t or C_t sequences (˛ = 2, 3, 4, 6, 8, 10, 14), T_t sequences (˛ = 2, 3, 4, 6, 8, 10), and G_t sequences (t = 2, 4) were measured in phosphate buffered solvents containing 30, 70, and 120 mM Na⁺. For dumbbells with loops comprised of at least three nucleotides, stability is inversely proportional to end-loop size. Dumbbells with loops comprised of only two nucleotide bases generally have lower stabilities than dumbbells with three base nucleotide loops. Experimental melting curves were analyzed in terms of the numerically exact (multistate) statistical thermodynamic model of DNA dumbbell melting previously described (T. M. Paner, M. Amaratunga & A. S. Benight (1992), Biopolymers 32, 881). Theoretically calculated melting curves were fitted to experimental curves by simultaneously adjusting model parameters representing statistical weights of intramolecular hairpin loop and single-strand circle states. The systematically determined empirical parameters provided evaluations of the energetics of hairpin loop formation as a function of loop size, sequence, and salt environment. Values of the free energies of hairpin loop formation ΔG_loop(n > t) and single-strand circles, ΔG_cir(N) as a function of end-loop size, t = 2-14, circle size, N = 32 + 2_t, and loop sequence were obtained. These quantities were found to depend on end-loop size but not loop sequence. Their empirically determined values also varied with solvent ionic strength. Analytical expressions for the partition function Q(T) of the dumbbells were evaluated using the empirically evaluated best-fit loop parameters. From Q(T), the melting transition enthalpy ΔH, entropy ΔS, and free energy ΔG, were evaluated for the dumbbells as a function of end-loop size, sequence, and [Na⁺]. Since the multistate analysis is based on the numerically exact model, and considers a statistically significant number of theoretically possible partially melted states, it does not require prior assumptions regarding the nature of the melting transition, i.e., whether or not it occurs in a two-state manner. For comparison with the multistate analysis, thermodynamic transition parameters were also evaluated directly from experimental melting curves assuming a two-state transition and using the graphical van't Hoff analysis. Comparisons between results of the multistate and two-state analyses suggested dumbbells with loops comprised of six or fewer residues melted in a two-state manner, while the melting processes for dumbbells with larger end-loops deviate from two-state behavior.Dependence of thermodynamic parameters on[Na⁺] as a function of loop size suggests single-strand end-loops have different counterion binding properties than the melted circle. Results are compared with those obtained in an earlier study of dumbbells with the slightly different stem sequence 5'-G-C-A-T-A-G-A-T-G-A-G-A-A-T-G-C-3' linked on the ends by T loops (˛ = 2,3,4,6,8,10,14).© 1996 John Wiley &Sons, Inc.     

Thermodynamics of melting of the circular dumbbell d〈pCGC-TT-GCG-TT〉

The conformational behavior of DNA minihairpin loops is sensitive to the directionality of the base pair that closes the loop. Especially tailored circular dumbbells, consisting of a stem of three Watson–Crick base pairs capped on each side with a minihairpin loop, serve as excellent model compounds by means of which deeper insight is gained into the relative stability and melting properties of hairpin loops that differ only in directionality of the closing pair: C-G vs G-C. For this reason the thermodynamic properties of the circular DNA decamers 5′-d〈pCGC-TT-GCG-TT〉-3′( I ) and reference compounds 5′-d〈pGGC-TT-GCC-TT≤-3′( II ) and 5′-d(GCG-TC-CGC)-3′( III ) are studied by means of nmr spectroscopy. Molecules I and II adopt dumbbell structures closed on both sides by a two-membered hairpin hop. At low temperature I consists of a mixture of two slowly exchanging forms, denoted L2L2 and L2L4 . The low-temperature L2L2 form is the fully intact minihairpin structure with three Watson–Crick C-G base pairs. The high-temperature form, L2L4 ,contains a partially disrupted closing G-C base pair in the 5′-GTTC-3′ loop, with the cytosine base placed in a syn orientation. The opposite 5′-CTTG-3′ loop remains stable. A study of the noncircular hairpin structure III shows similar conformational behavior for the 5′-GTTC-3′ loop as found in I a syn orientation for C(6) and two slowly exchanging imino proton signals for G(3). The melting point T_m of II was estimated to lie above 365 K. The T_m value of the duplex stem and the 5′-CTTG-3′ loop of the L2L4 form ofIis 352 ± 2 K. The ΔH° is calculated as ?89 ± 10 kJ/mol. The T_m value determined for the individual residues of the 5′-GTTC-3′ loop lies 4°–11° lower. The enthalpy ΔH° of melting the thymine residues in the 5′-GTTC-3′ loop is calculated to be -61± 7 kJ/mol. Thermodynamic data of the equilibrium between the slowly exchanging two- and four-membered loop conformers of I reveal an upper limit for ΔH° of +30 kJ/mol in going from a two-memberedto a four-membered loop, in agreement with the enthalpy difference of +28 k.j/mol between the two loops at the T_m midpoint. For hairpin III the upper limit for ΔH° going from a two-membered to a four-membered loop amounts to ±21 kJ/mol. The mutual exchange rate between the L2 and L4 form in III is estimated as 13.6 s^?1. Our results clearly suggest that small four-way DNA junctions(model for immobilized Holliday junctions) can be designed that consist of a single DNA strandthat features -CTTG-caps on three of the four arms of the junction. © 1995 John Wiley & Sons, Inc.     

Slow conformational exchange in DNA minihairpin loops: A conformationalstudy of the circular dumbbell d〈pCGC-TT-GCG-TT〉

In recent years various examples of highly stable two-residue hairpin loops (miniloops) in DNA have been encountered. As the detailed structure and stability of miniloops appear to be determined not only by the nature and sequence of the two bases in the loop, but also by the closing base pair, it is desirable to carry out in-depth studies of especially designed small model DNA compounds. Therefore, a circular DNA dumbbell-like molecule is tailored to consist of a stem of three Watson–Crick base pairs, flanked on each side by a minihairpin loop. The resulting circular DNA decanter 5′-d〈pCGC- TT-GCG- TT〉 -3′ ( I ) is studied in solution by means of nmr spectroscope. At a temperature of 269 K the molecule occurs in a 50/50 mixture of two dumbbell structures (denoted L2L2 and L2L4). L2L2 contains three Watson–Crick C-G base pairs and two two-residue loops (H2-family type) in opposite parts of the molecule. On raising the temperature from 269 to 314 K. The L2L4 conformer becomes increasingly dominant (95% at 314 K). This conformer has a partially disrupted closing G-C base pair in the 5′-GTTC-3′ loop with only one remaining solvent-accessible hydrogen bond between NH_α of the cytosine C(1) and O6 of the guanine G(8), whereas the opposite 5′-CTTG-3′ loop remains stable. The disruption of the C(1)-G(8) base pair in the L2L4 form is correlated with the presence of a syn orientation for the C(1) base at the 5′-3′ loop-stem junction in the 5′-GTTC-3′ loop. The two conformers. L2L2 and L2L4, occur in slow equilibrium (2–20 s^?1). Moderate line broadening of specific ¹H, ¹³C, and ³¹P resonances of residues C(1), G(8), T(9), and T(10) at low temperatures, due to chemical exchange between L2L2 and L2L4, show that the interconversion from an anti to syn conformer in residue C(1) has a small local effect on the structure of the dumbbell. T₁ relaxation measurements, chemical-shift considerations, and complete hand-shape calculations of the exchange process of the G(8) imino proton reveal a possibility for the existence of multiconformational slates in the anti–syn equilibrium. © 1995 John Wiley & Sons, Inc.     

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.     

EXTRA STABLE 2′,5′-LINKED RNA LOOPS

We prepared hairpins that differ in the connectivity of phosphodiester linkages in the loop (RNA vs 2′, 5′-RNA). We find that the stability of the extra stable RNA hairpin 5′-rGGAC(UUCG)GUCC-3′ is the same as that observed for the hairpin containing a 2′,5′RNA loop, i.e. 5′-rGGAC(UUCG)GUCC-3′ (where UUCG = U_2′p5′U_2′p5′ C_2′p5′G_2′p5′). Also significant is the finding that when the stem is duplex DNA, duplex 2′,5′-RNA, or DNA:2′,5′-RNA, hairpins with the UUCG loop are more stable than those with UUCG loop.     

Properties and Anti-HIV Activity of Nicked Dumbbell Oligonucleotides

Abstract

We have designed a new type of oligodeoxyribonucleotide. These oligodeoxyribonucleotides form two hairpin loop structures with base pairs (sense and antisense) in the double helical stem at the 3′ and 5′-ends (nicked dumbbell oligonucleotides). The nicked dumbbell oligonucleotides are molecules with free ends that are more resistant to exonuclease attack. Furthermore, the nicked dumbbell oligonucleotide containing phosphorothioate (P=S) bonds in the hairpin loops has increased nuclease resistance, as compared to the unmodified nicked oligonucleotide. The binding of the nicked dumbbell oligonucleotide to RNA is lower than that of a single-stranded DNA. We also describe the anti-HIV activity of nicked dumbbell oligonucleotides.

     

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.     

Improved Targeting of the Flanks of a DNA Stem Using α-Oligodeoxynucleotides.-The Enhanced Effect of an Intercalator

Abstract

2′-Deoxy-5′-0-(4,4′-dimethoxytrityl)-5-methyl-N ⁴-(1-pyrenylmethyl)-α-cytidine (5) was prepared by reaction of 1-pyrenylmethylamine with an appropriate protected 4-(l,2,4-triazolyl)-α-thymidine derivative 3 which was synthesized from 5-O-DMT protected α-thymidine 1. Aminolysis of 3 afforded 3′-O-acetyl-2′-deoxy-5′-O-(4,4′-dimethoxytrityl)-5-methyl-α-cytidine (8). Benzoylation of 8 and removal of acetyl afforded N ⁴-benzoyl-2-deoxy-5–0-(4,4′-dimethoxytrityl)-5-methyl-α-cytidine (10). The amidites of compounds 5and 10 were prepared and used in α-oligonucleotide synthesis. DNA three-way junction (TWJ) is stabilized when an α-ODN is used for targeting the dangling flanks of the stem in a DNA hairpin. Further stabilization of the TWJ is observed when 5 is inserted into the α-ODN at the junction region.

     

Structure and Conformation of the Duplex Consensus Acceptor Exon: Intron Junction d [(CpTpApCpApGpGpT) (ApCpCpTpGpTpApG)] deduced from High-Field 1H-NMR of Non-Exchangeable and Imino Protons

Abstract

The complementary consensus acceptor exon:intron junction d(ApCpCpTpGpTpApG) has been synthesized by a modified phosphotriester method. The non self-complementary octamer exists in the random coil form in aqueous buffer at 20°C as evidenced by temperature variable ¹H-NMR and NOE measurements. The non-exchangeable proton assignments were secured using a combination of techniques including two-dimensional COSY, NOESY and ¹H-¹H-INADEQUATE. The octamer was annealed with the primary consensus sequence d(CpTpApCpApGpGpT). Confirmation of complete duplex formation was confirmed by detection and assignment of imino protons in D₂O:H₂O mixtures. Assignment of the nonexchangeable proton signals in the duplex consensus junction was then secured by a combination of two-dimensional COSY correlations, NOESY and NOE experiments. Determination of individual vicinal coupling constants in the component deoxyribose moieties permitted deduction of the population of S conformations in this sequence. It is concluded that the consensus acceptor junction exists in solution in a conformation belonging to the B family, and that the bases are oriented anti. In addition the deoxyribose moieties in the 5′ regions exist predominantly in the S form (2′endo—3′exo) whereas those residues on or adjacent to the junction on the primary strand show more N character (2′exo—3′endo). The contiguous bases A₅-G₆ (adjacent to the junction) and A₁₅-G₁₆ are stacked more closely than the other neighbor bases in this duplex sequence. These subtle structural and conformational differences in the exon:intron junction may serve as recognition signals for these critical sites in the genome.     

Structure of Three-Way DNA Junctions 1. Non-Planar DNA Geometry

Abstract

Three-way junctions were obtained by annealing two synthetic DNA-oligomers. One of the strands contains a short palindrome sequence, leading to the formation of a hairpin with four base pairs in the stem and four bases in the loop. Another strand is complementary to the linear arms of the first hairpin-containing strand. Both strands were annealed to form a three-way branched structure with sticky ends on the linear arms. The branched molecules were ligated, and the ligation mixture was analysed on a two-dimensional gel in conditions which separated linear and circular molecules. Analysis of 2D-electrophoresis data shows that circular molecules with high mobility are formed. Formation of circular molecules is indicative of bends between linear arms. We estimate the magnitude of the angle between linear arms from the predominant size of the circular molecules formed. When the junction-to-junction distance is 20–21 bp, trimers and tetramers are formed predominately, giving an angle between linear arms as small as 60–90°. Rotation of the hairpin position in the three- way junction allowed us to measure angles between other arms, yielding similar values. These results led us to conclude that the three-way DNA junction possesses a non-planar pyramidal geometry with 60–90° between the arms. Computer modeling of the three-way junction with 60° pyramidal geometry showed a predominantly B-form structure with local distortions at the junction points that diminish towards the ends of the helices. The size distributions of circular molecules are rather broad indicating a dynamic flexibility of three-way DNA junctions.     

Solution structure of the HIV-1 exon splicing silencer 3

Alternative splicing of the human immunodeficiency virus type 1 (HIV-1) genomic RNA is necessary to produce the complete viral protein complement, and aberrations in the splicing pattern impair HIV-1 replication. Genome splicing in HIV-1 is tightly regulated by the dynamic assembly/disassembly of trans host factors with cis RNA control elements. The host protein, heterogeneous nuclear ribonucleoprotein (hnRNP) A1, regulates splicing at several highly conserved HIV-1 3′ splice sites by binding 5′-UAG-3′ elements embedded within regions containing RNA structure. The physical determinants of hnRNP A1 splice site recognition remain poorly defined in HIV-1, thus precluding a detailed understanding of the molecular basis of the splicing pattern. Here, the three-dimensional structure of the exon splicing silencer 3 (ESS3) from HIV-1 has been determined using NMR spectroscopy. ESS3 adopts a 27-nucleotide hairpin with a 10-bp A-form stem that contains a pH-sensitive A⁺C wobble pair. The seven-nucleotide hairpin loop contains the high-affinity hnRNP-A1-responsive 5′-UAGU-3′ element and a proximal 5′-GAU-3′ motif. The NMR structure shows that the heptaloop adopts a well-organized conformation stabilized primarily by base stacking interactions reminiscent of a U-turn. The apex of the loop is quasi-symmetric with UA dinucleotide steps from the 5′-GAU-3′ and 5′-UAGU-3′ motifs stacking on opposite sides of the hairpin. As a step towards understanding the binding mechanism, we performed calorimetric and NMR titrations of several hnRNP A1 subdomains into ESS3. The data show that the UP1 domain forms a high-affinity (K_d = 37.8 ± 1.1 nM) complex with ESS3 via site-specific interactions with the loop.     

Common Structural Features of UUCG and UACG Tetraloops in Very Short Hairpins Determined by UV Absorption,Raman, IR and NMR Spectroscopies

Abstract

Thermodynamic and structural properties of two UNCG tetraloops in very short hairpin octamers, 5′-r (GCUUCGGC)-3′ and 5′-r (GCUACGGC)-3′. have been studied by means of various physical techniques. Melting profiles of both octamers, obtained from UV absorption spectra taken as a function of temperature, are consistent with a monophasic, progressive and completely reversible order-to-disorder transition and confirm their unusual structural stability (T_m>51^° C). The ¹H, ¹³C and ³¹P NMR chemical shifts and coupling constants of the UACG loop nucleotides are comparable with those reported previously for UUCG loops, i.e. 2′-endo/anti conformation of the second and third nucleotide of the loop as well as the syn orientation of the ultimate guanine base and the A-type double helical conformation of the hairpin stem. Simulation of quantitative NOESY volumes shows that the UACG octamer adopts a very rigid compact structure which is well represented by an average order parameter of 0.9. Three base-pairs and four additional strong hydrogen bonds are undoubtedly responsible for such limited flexibility. Raman and infrared spectra as a function of temperature reflect the order-to-disorder transition, as well. Vibrational conformational markers in low temperature spectra of both octamers indicate the hairpin structure as the major conformer in aqueous phase. These spectra further support the structural features of most of the nucleotides involved in the tetraloops and clearly demonstrate the structural similarities of the phosphodiester backbone in both hairpins. Consequently, on the basis of all present results, one can deduce that the conformational features of the UUCG and UACG tetraloops seem to be inherent to the UNCG type tetraloops, regardless of either the nature of the tetraloop second base or the stem length.     

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.     

The complete nucleotide sequence of a 16S ribosomal RNA gene from tobacco chloroplasts: Recombinant plasmid; sequence homology; stem and loop structure

The complete nucleotide sequence of a 16S ribosomal RNA gene from tobacco chloroplasts has been determined. This nucleotide sequence has 96% homology with that of maize chloroplast 16S rRNA gene and 74% homology with that of Escherichia coli16S gene.The 3′ terminal region of this gene contains the sequence ACCTCC which is complementary to sequences found at the 5′ termini of prokaryotic mRNAs.The large stem and loop structure can be constructed from the sequences surrounding the 5′ and 3′ ends of the 16S gene. These observations demonstrate the prokaryotic nature of chloroplast 16S rRNA.     

Detection of specific sequences among DNA fragments separated by gel electrophoresis.

Ribosomal RNA and precursor ribosomal RNA from at least one representative of each vertebrate class have been analyzed by electron microscopic secondary structure mapping. Reproducible patterns of hairpin loops were found in both 28 S ribosomal and precursor ribosomal RNA, whereas almost all the 18 S ribosomal RNA molecules lack secondary structure under the spreading conditions used. The precursor ribosomal RNA of all species analyzed have a common design. The 28 S ribosomal RNA is located at or near the presumed 5′-end and is separated from the 18 S ribosomal RNA region by the internal spacer region. In addition there is an external spacer region at the 3′-end of all precursor ribosomal RNA molecules. Changes in the length of these spacer regions are mainly responsible for the increase in size of the precursor ribosomal RNA during vertebrate evolution. In cold blooded vertebrates the precursor contains two short spacer regions; in birds the precursor bears a long internal and a short external spacer region, and in mammals it has two long spacer regions. The molecular weights, as determined from the electron micrographs, are 2·6 to 2·8 × 10⁶ for the precursor ribosomal RNA of cold blooded vertebrates, 3·7 to 3·9 × 10⁶ for the precursor of birds, and 4·2 to 4·7 × 10⁶ for the mammalian precursor. Ribosomal RNA and precursor ribosomal RNA of mammals have a higher proportion of secondary structure loops when compared to lower vertebrates. This observation was confirmed by digesting ribosomal RNAs and precursor ribosomal RNAs with single-strandspecific S₁ nuclease in aqueous solution. Analysis of the double-stranded, S₁-resistant fragments indicates that there is a direct relationship between the hairpin loops seen in the electron microscope and secondary structure in aqueous solution.     

Primary structure of E. coli alanine transfer RNA: relation to the yeast phenylalanyl tRNA synthetase recognition site

Nucleotide sequence comparison of tRNAs aminoacylated by yeast phenylalanyl tRNA synthetase (PRS) have lead to the proposal that the specific nucleotides of the dihydrouridine (diHU) stem region and adenosine at the fourth position from the 3′ end are involved in the PRS recognition site. Kinetic analysis and enzymatic methylation have shown that the size of the diHU loop and the methylation of guanine at position 10 from the 5′ end both directly affect the PRS aminoacylation kinetics. $\text{E. coli}$ tRNA₁^A1a, which is aminoacylated by PRS, should therefore have 1- the specific nucleotides of the diHU stem region and, 2- adenosine at position 4 from the 3′ end. The PRS aminoacylation kinetics of this tRNA indicates that this molecule 3- has a diHU loop of 8 nucleotides and 4- has an unmethylated guanine at position 10 from the 5′ end. We report here the complete sequence of $\text{E. coli}$ tRNA₁^A1a and confirmation of each of these four predictions.     

The Telomeric dG(GT)4G Sequence Can Adopt a Parallel-Stranded Double Helical Conformation

Abstract

Oligonucleotides 3′-d(GTGTGTGTGG)-L-d(GGTGTGTGTG)-3′ (hp-GT) and 3′- d(G^4STG^4STG^4STG^4STGG)-L-d(GGTGTGTGTG)-3′ (hp-SGT), (L=(CH₂CH₂O)₃), were shown by use of several optical techniques to form a novel parallel-stranded (ps) intramolecular double helix with purine-purine and pyrimidine-pyrimidine base pairing. The rotational relaxation time of hp-GT was similar to that of a 10-bp reference duplex, and the fraction of unpaired bases was determined to be ～ 7%, testifying to the formation of an intramolecular double helical hairpin by the sequence under the given experimental conditions. A quasi-two- state mode of ps-double helix formation was validated, yielding a helix-coil transition enthalpy of ?135±5 kJ/mol. The G-G and T·T (or ^4ST·T) base pair configurations and conformational parameters of the double helix were derived with molecular modeling by force field techniques. Repetitive d(GT) sequences are abundant in telomers of different genomes and in the regulatory regions of genes. Thus, the observed conformational potential of the repetitive d(GT) sequence may be of importance in the regulation of cell processes.     

Hybridization of single-stranded DNA targets to immobilized complementary DNA probes: comparison of hairpin versus linear capture probes

A microtiter-based assay system is described in which DNA hairpin probes with dangling ends and single-stranded, linear DNA probes were immobilized and compared based on their ability to capture single-strand target DNA. Hairpin probes consisted of a 16 bp duplex stem, linked by a T₂-biotin·dT-T₂ loop. The third base was a biotinylated uracil (U_B) necessary for coupling to avidin coated microtiter wells. The capture region of the hairpin was a 3′ dangling end composed of either 16 or 32 bases. Fundamental parameters of the system, such as probe density and avidin adsorption capacity of the plates were characterized. The target DNA consisted of 65 bases whose 3′ end was complementary to the dangling end of the hairpin or to the linear probe sequence. The assay system was employed to measure the time dependence and thermodynamic stability of target hybridization with hairpin and linear probes. Target molecules were labeled with either a 5′-FITC, or radiolabeled with [γ-³³P]ATP and captured by either linear or hairpin probes affixed to the solid support. Over the range of target concentrations from 10 to 640 pmol hybridization rates increased with increasing target concentration, but varied for the different probes examined. Hairpin probes displayed higher rates of hybridization and larger equilibrium amounts of captured targets than linear probes. At 25 and 45°C, rates of hybridization were better than twice as great for the hairpin compared with the linear capture probes. Hairpin–target complexes were also more thermodynamically stable. Binding free energies were evaluated from the observed equilibrium constants for complex formation. Results showed the order of stability of the probes to be: hairpins with 32 base dangling ends > hairpin probes with l6 base dangling ends > 16 base linear probes > 32 base linear probes. The physical characteristics of hairpins could offer substantial advantages as nucleic acid capture moieties in solid support based hybridization systems.     

A possible novel interaction between the 3′-end of 18 S ribosomal RNA and the 5'-leader sequence of many eukaryotic messenger RNAs

A novel interaction between the 5′-untranslated region of eukaryotic messenger RNAs and non-contiguous sequences in the 18 S ribosomal RNA is proposed. The small ribosomal RNA contains, at its 3′-terminus, a heavily conserved hairpin structure. It is suggested that mRNA 5′-leader sequence stabilises this structure by interacting with other conserved nucleotides which flank it. Sequences closely related to the required sequence (A—U—C—C—A—C—C) occur quite commonly in eukaryotic mRNAs and are often found immediately upstream from the AUG-codon. This interaction may have a role in the events which lead up to the initiation of protein synthesis.