Modification of tumour growth with a defined glycoprotein antigen

A single natural RNA modification can destabilize a U•A-T-rich RNA•DNA-DNA triple helix

Recent studies suggest noncoding RNAs interact with genomic DNA, forming RNA•DNA-DNA triple helices, as a mechanism to regulate transcription. One way cells could regulate the formation of these triple helices is through RNA modifications. With over 140 naturally occurring RNA modifications, we hypothesize that some modifications stabilize RNA•DNA-DNA triple helices while others destabilize them. Here, we focus on a pyrimidine-motif triple helix composed of canonical U•A-T and C•G-C base triples. We employed electrophoretic mobility shift assays and microscale thermophoresis to examine how 11 different RNA modifications at a single position in an RNA•DNA-DNA triple helix affect stability: 5-methylcytidine (m⁵C), 5-methyluridine (m⁵U or rT), 3-methyluridine (m³U), pseudouridine (Ψ), 4-thiouridine (s⁴U), N ⁶-methyladenosine (m⁶A), inosine (I), and each nucleobase with 2'-O-methylation (Nm). Compared to the unmodified U•A-T base triple, some modifications have no significant change in stability (Um•A-T), some have ∼2.5-fold decreases in stability (m⁵U•A-T, Ψ•A-T, and s⁴U•A-T), and some completely disrupt triple helix formation (m³U•A-T). To identify potential biological examples of RNA•DNA-DNA triple helices controlled by an RNA modification, we searched RMVar, a database for RNA modifications mapped at single-nucleotide resolution, for lncRNAs containing an RNA modification within a pyrimidine-rich sequence. Using electrophoretic mobility shift assays, the binding of DNA-DNA to a 22-mer segment of human lncRNA Al157886.1 was destabilized by ∼1.7-fold with the substitution of m⁵C at known m⁵C sites. Therefore, the formation and stability of cellular RNA•DNA-DNA triple helices could be influenced by RNA modifications.

Binding properties of chiral ruthenium(II) complexes Λ- and Δ-[Ru(bpy)2dppz-11-CO2Me]2+ toward the triplex RNA poly(U)•poly(A)*poly(U)

Two chiral ruthenium(II) complexes containing ligand dppz-CO₂Me (dppz-11-CO₂Me = dipyrido[3,2-a,2',3'-c]phenazine-11-carboxylic acid methyl ester), Δ-[Ru(bpy)₂dppz-11-CO₂Me]²⁺ (bpy = 2,2'-bipyridine; Δ-1) and Λ-[Ru(bpy)₂dppz-11-CO₂Me]²⁺ (Λ-1), were synthesized and characterized. The binding of the two enantiomers with the triplex RNA poly(U)•poly(A)*poly(U) was carried out by various biophysical techniques. Analysis of the absorption and fluorescence features indicates that the binding strengths of the two enantiomers toward the triplex RNA differ only slightly from each other. The total increase in viscosity and shape of the curves for the triplex RNA with Λ-1 is similar to that with Δ-1, suggesting the binding modes of two enantiomers with the triplex RNA are intercalation. Thermal melting measurements indicate that the stabilization effects clearly depended on the concentrations of Λ-1 and Δ-1. However, the third-strand stabilizing effect of Δ-1 dramatically differs from that of Λ-1 when they interact with the chiral environment of the RNA triple at pH = 7.0 and [Na⁺] = 35 mM. Combined with the CD (CD = circular dichroism) variations of the triplex RNA with either Λ-1 or Δ-1, the reason for their different triplex stabilization effects may originate from the two enantiomers through different orientations intercalating into nucleobases of the triplex. In addition, effects of higher ionic strengths on the triplex stabilization in the absence and presence of the two enantiomers have also been studied. The results presented here may be useful for understanding the binding properties of the triplex RNA with small molecule, particularly chiral ruthenium(II) complexes.

FTIR and UV spectroscopy studies of triplex formation between alpha-oligonucleotides with non-ionic phoshoramidate linkages and DNA targets

The triplexes formed by pyrimidine alpha-oligodeoxynucleotides, 15mers alpha dT(15) or 12mers alpha dCT having dimethoxyethyl (PNHdiME), morpholino (PMOR) or propyl (PNHPr) non-ionic phosphoramidate linkages with DNA duplex targets have been investigated by UV and FTIR spectroscopy. Due to the decrease in the electrostatic repulsion between partner strands of identical lengths all modifications result in triplexes more stable than those formed with unmodified phosphodiester beta-oligodeoxynucleotides (beta-ODNs). Among the alpha-ODN third strands having C and T bases and non-ionic phosphoramidate linkages (alpha dCTPN) the most efficient modification is (PNHdiME). The enhanced third strand stability of the alpha dCTPN obtained as diastereoisomeric mixtures is attenuated by the steric hindrance of the PMOR linkages or by the hydrophobicity of the PNHPr linkages. All alpha dCTPN strands form triplexes even at neutral pH. In the most favorable case (PNHdiME), we show by FTIR spectroscopy that the triplex formed at pH 7 is held by Hoogsteen T*A.T triplets and in addition by an hydrogen bond between O6 of G and C of the third strand (Tm = 30 degrees C). The detection of protonated cytosines is correlated at pH 6 with a high stabilization of the triplex (Tm = 65 degrees C). While unfavorable steric effects are overcome with alpha anomers, the limitation of the pH dependence is not completely suppressed. Different triplexes are evidenced for non pH dependent phosphoramidate alpha-thymidilate strands (alpha dT(15)PN) interacting with a target duplex of identical length. At low ionic strength and DNA concentration we observe the binding to beta dA(15) either of alpha dT(15)PN as duplex strand and beta dT(15) as third strand, or of two hydrophobic alpha dT(15)PNHPr strands. An increase in the DNA and counterion concentration stabilizes the anionic target duplex and then the alpha dT(15)PN binds as Hoogsteen third strand.

Molecular dynamics simulation study of DNA triplex formed by mixed sequences in solution

The unrestrained molecular dynamics simulation of the triple helical DNA with mix sequences d(GACTGGTGAC).d(CTGACCACTG)*d (GACTGGTGAC), using the particle mesh Ewald sum, is presented here. The Ewald summation method effectively eliminates the usualcut-of of the long range interactions and allowed us to evaluate the full effect of the electrostatic forces. The AMBER5.0 force field has been used during the simulation in solvent. The MD results support a dynamically stable model of DNA triplex over the entire length of the trajectory. The duplex structure assumes the conformation, which is very close to B-DNA. In mixed sequences the purine bases occurs in both strand of DNA duplex. The bases of third strand do not favor the Hoogsteen or/and reverse Hoogsteen type of Hydrogen bonding but they form hydrogen bonds with the bases of both the strand of DNA duplex. The orientation of the third strand is parallel to one of the strand of duplex and all nucleotides (C, A, G & T) show isomorphic behavior with respect to the DNA duplex. The conformation of all the three strands is almost same except few exceptions. Due to interaction of third strand the conformational change in the duplex structure and a finite amount of displacement in the W-C base pairs have been observed. The conformational variation of the back bone torsion angles and helicoidal parameters, groove widths have been discussed. The sequence dependent effects on local conformation, helicoidal and morphological structure, width of the grooves of DNA helix may have important implication for understanding the functional energetics and specificity of interactions of DNA and its triplexes with proteins, pharmaceutical agents and other ligands.

Structure of Poly (U).poly (A).poly (U)

The molecular structure of poly (U).poly (A).poly (U) has been determined and refined using the continuous x-ray intensity data on layer lines in the diffraction pattern obtained from an oriented fiber of the RNA. The final R-value for the preferred structure is 0.24, far lower than that for the plausible alternatives. The polymer forms an 11-fold right-handed triple-helix of pitch 33.5A and each base triplet is stabilized by Crick-Watson-Hoogsteen hydrogen bonds. The ribose rings in the three strands have C3'-endo, C2'-endo and C2'-endo conformations, respectively. The helix derives additional stability through systematic interchain hydrogen bonds involving ribose hydroxyls and uracil bases. The relatively grooveless cylindrical shape of the triple-helix is consistent with the lack of lateral organization.

The integral divalent cation within the intermolecular purine*purine. pyrimidine structure: a variable determinant of the potential for and characteristics of the triple helical association

In vitro assembly of an intermolecular purine*purine.pyrimidine triple helix requires the presence of a divalent cation. The relationships between cation coordination and triplex assembly were investigated, and we have obtained new evidence for at least three functionally distinct potential modes of divalent cation coordination. (i) The positive influence of the divalent cation on the affinity of the third strand for its specific target correlates with affinity of the cation for coordination to phosphate. (ii) Once assembled, the integrity of the triple helical structure remains dependent upon its divalent cation component. A mode of heterocyclic coordination/chelation is favorable to triplex formation by decreasing the relative tendency for efflux of integral cations from within the triple helical structure. (iii) There is also a detrimental mode of base coordination through which a divalent cation may actively antagonize triplex assembly, even in the presence of other supportive divalent cations. These results demonstrate the considerable impact of the cationic component, and suggest ways in which the triple helical association might be positively or negatively modulated.

Effect of selective substitution of 5-bromocytosine on conformation of DNA triple helices

Three triplex DNAs containing 5-bromocytosine[BrC] were studied by vibrational spectroscopy and molecular modelling. Firstly, three oligodeoxypyrimidines of 5'-(TC)3-T4-(BrCT)3 [CBrC], 5'-(TBrC)3-T4-(CT)3 [BrCC] and 5'-(TBrC)3-T4-(BrCT)3 [BrCBrC] were synthesized and then reacted with an oligodeoxypurine of 5'-(AG)3 at pH=4.5 in phosphate buffer respectively to form three comparative hairpin triplex named CY,YC and YY. The results of FT-Raman and IR revealed that YY is almost in A-like form, CY and YC are combinations of A-like form and B-like form, but A-form dominates in CY while B-form is equivalent as A-form in YC. The result is consistent with the theoretical analysis.

Free energy of the binding of uridylic acid oligomers with double stranded poly(A) · poly(U)

The binding parameters (K, omega) and the free energy (DeltaG(0)) of triple helix formation have been estimated for complexes of oligo(U)(n) (n = 5, 7-10) with poly(A) . poly(U) on the basis of hypochromicity measurements. The data were treated according to the formula of McGhee and von Hippel [J. Mol. Biol. 86 (1974) 469] by a computer program ALAU [H. Schütz et al., Stud. Biophys. 104 (1984) 23] which takes absorbancies and total concentrations as input. In 1 mM cacodylate buffer pH 7.0 with 10 mM NaCl and 10 mM MgCl(2) at 5 degrees C the free energy of contiguous binding was found to be a linear function of the oligomer length with a slope of DeltaG(c,U)(0) = -0.72 (+/-0.03) kcal x mol(-1) per nucleotide. The mean cooperativity coefficient (omega) was 24.5 (+/- 5.6), and the corresponding free energy of interaction between the neighbouring oligonucleotides in the third strand was DeltaG(0(omega)) = -1.74 (+/-0.13) kcal x mol(-1).

Structural features and stability of an RNA triple helix in solution

A 30 nt RNA with a sequence designed to form an intramolecular triple helix was analyzed by one-and two-dimensional NMR spectroscopy and UV absorption measurements. NMR data show that the RNA contains seven pyrimidine-purine-pyrimidine base triples stabilized by Watson-Crick and Hoogsteen interactions. The temperature dependence of the imino proton resonances, as well as UV absorption data, indicate that the triple helix is highly stable at acidic pH, melting in a single sharp transition centered at 62 degrees C at pH 4.3. The Watson-Crick and Hoogsteen pairings are disrupted simultaneously upon melting. The NMR data are consistent with a structural model where the Watson-Crick paired strands form an A-helix. Results of model building, guided by NMR data, suggest a possible hydrogen bond between the 2' hydroxyl proton of the Hoogsteen strand and a phosphate oxygen of the purine strand. The structural model is discussed in terms of its ability to account for some of the differences in stability reported for RNA and DNA triple helices and provides insight into features that are likely to be important in the design of RNA binding compounds.

Prospects for the therapeutic use of antigene oligonucleotides

An outgrowth of classic nucleic acid interaction studies, oligonucleotide-directed triple helix formation is a unique method for creating highly specific chemical ligands that recognize and bind to particular sequences of duplex DNA. Under permissive conditions, these oligonucleotide-based compounds can approach or exceed the binding affinity and sequence specificity of natural DNA-binding proteins. Triple helix recognition has been found to be useful in certain cell-free applications including precise chromosome fragmentation. It has been proposed that such oligonucleotides could also form the basis for gene-targeted (antigene) drugs that might repress transcription from undesired genes in living cells. However, current strategies for oligonucleotide-directed triple helix formation suffer from important constraints involving requirements for stabilizing binding conditions, restrictions on permitted target sequences, and inefficient nuclear delivery of oligonucleotides. Implementation of oligonucleotide-directed triple helix formation as a viable approach to cancer therapy must therefore await clever solutions to a series of fascinating problems.

Stability and cooperativity of nucleic acid base triplets

Geometries and stabilities of various base triplets have been studied using ab initio quantum chemical methods. Their optimized geometries are determined using the STO-3G basis set, and those of Hoogsteen and reverse Hoogsteen base pairs are evaluated with the 4-31G basis set. Moreover, the preferred hydrogen bond patterns of the bases in triple helices are discussed. A cooperative effect for base pairing in triplets is presented, and it can be either positive or negative. Almost all base triplets that contain Watson-Crick G:C base pairs show a positive cooperativity. Conversely, the base triplets with Watson-Crick A:T base pairs mostly display a negative cooperativity. The interaction energies of base triplets are reported and the relative stabilities of base triplets are found as follows: A+.GC > C+.GC(H) > C+.GC(rH) > G.GC(H) > G.GC(rH) > A.GC > T.AT(rH) > U.AU(H) > U.AT(H) > A.AT > G.AT > T.AT(m) > G.TA(2) > G.TA(1) H and rH denote the Hoogsteen and reverse Hoogsteen positions of the third base that would lead to parallel and antiparallel orientations respectively of the third chain with respect to the Watson-Crick paired purine chain. 'm' denotes the middle pairing scheme, in which the third base hydrogen bonds to both bases of Watson-Crick pair.

Molecular dynamics investigations of DNA triple helical models: unique features of the Watson-Crick duplex

We have built computer models of triple helical structures with a third poly(dT) strand Hoogsteen base paired to the major groove of a poly(dA).poly(dT) Watson-Crick (WC) base-paired duplex in the canonical A-DNA as well as B-DNA. For the A-DNA form, the sugar-phosphate backbone of the third strand intertwines and clashes with the poly(dA) strand requiring a radical alteration of the duplex to access the hydrogen bonding sites in the major groove. In contrast, when the duplex was in the canonical B-DNA form, the third strand was readily accommodated in the major groove without perturbing the duplex. The triple helical model, with the duplex in the B-DNA form, was equilibrated for 400ps using molecular dynamics simulations including water molecules and counter-ions. During the entire simulations, the deoxyriboses of the adenine strand oscillate between the S-type and E-type conformations. However, 30% of the sugars of the thymine strands-II & III switch to the N-type conformation early in the simulations but return to the S-type conformation after 200ps. In the equilibrium structure, the WC duplex portion of the triplex is unique and its geometry differs from both the A- or B-DNA. the deoxyriboses of the three strands predominantly exhibit S-type conformation. Besides the sugar pucker, the major groove width and the base-tilt are analogous to B-DNA, while the X-displacement and helical twist resemble A-DNA, giving a unique structure to the triplex and the Watson & Crick and Hoogsteen duplexes.

A possible family of B-like triple helix structures: comparison with the Arnott A-like triple helix

Recent experimental studies of the structure of triple helices show that their conformation in solution differs from the A-like structure derived from diffraction data on triple helix fibers by Arnott and co-workers. Here we show by means of molecular modeling that a family of triple helix structures may exist with similar conformational energies, but with a variety of sugar puckers. The characteristics of these putative triple helices are analyzed for three different base sequences: (T.AxT)n, (C.GxC+)n, and alternating (C.GxC+/T.AxT)n. In the case of (C.GxC+)n triple helix, infrared and Raman spectra have been obtained and clearly reveal the existence of both N- and S-type sugars in solution. The molecular mechanics calculations allow us to propose a stereochemically reasonable model for this triple helix, in good agreement with the vibrational spectroscopy results.

Triple helical polynucleotidic structures: an FTIR study of the C+ .G. Ctriplet

Triple helixes containing one homopurine poly dG or poly rG strand and two homopyrimidine poly dC or poly rC strands have been prepared and studied by FTIR spectroscopy in H2O and D2O solutions. The spectra are discussed by comparison with those of the corresponding third strands (auto associated or not) and of double stranded poly dG.poly dC and poly rG.poly rC in the same concentration range and salt conditions. The triplex formation is characterized by the study of the base-base interactions reflected by changes in the spectral domain involving the in-plane double bond vibrations of the bases. Modifications of the initial duplex conformation (A family form for poly rG.poly rC, B family form for poly dG.poly dC) when the triplex is formed have been investigated. Two spectral domains (950-800 and 1450-1350 cm-1) containing absorption bands markers of the N and S type sugar geometries have been extensively studied. The spectra of the triplexes prepared starting with a double helix containing only riboses (poly rC+.poly rG.poly rC and poly dC+.poly rG.poly rC) as well as that of poly rC+.poly dG.poly dC present exclusively markers of the North type geometry of the sugars. On the contrary in the case of the poly dC+.poly dG.poly dC triplex both N and S type sugars are shown to coexist. The FTIR spectra allow us to propose that in this case the sugars of the purine (poly dG) strand adopt the S type geometry.

Triple helical polynucleotidic structures: sugar conformations determined by FTIR spectroscopy

Fourier Transform Infrared Spectra of triple stranded polynucleotides containing homopurine dA or rA and homopyrimidine dT or rU strands have been obtained in H2O and D2O solutions as well as in hydrated films at various relative humidities. The spectra are interpreted by comparison with those of double stranded helixes with identical base and sugar composition. The study of the spectral domain corresponding to in-plane double bond stretching vibrations of the bases shows that whatever the initial duplex characterized by a different IR spectrum (A family form poly rA.poly rU, heternomous form poly rA.poly dT, B family form poly dA.poly dT), the triplexes present a similar IR spectrum reflecting similar base interactions. A particular attention is devoted to the 950-800 cm-1 region which contains marker bands of the sugar conformation in the nucleic acids. In solution the existence of only N (C3'endo-A family form) type of sugar pucker is detected in poly rU.poly rA.poly rU and poly dt.poly rA.poly rU. On the contrary absorption bands characteristic of both N (C3'endo-A family form) and S (C2'endo-B family form) type sugars are detected for poly rU.poly rA.poly dT, poly rU.poly dA.poly dT and poly dT.poly rA.poly dT. Finally mainly S (C2'endo-B family form) type sugars are observed in poly dT.poly dA.poly dT.

The influence of Mg++ and Zn++ on polypurine-polypyrimidine multistranded helices

We have studied by X-ray diffraction fibres of complexes of polypurine-polypyrimidine with divalent cations. In the presence of Mg++, poly(dC) and poly(dG) form a very stable triple helix at neutral pH, based on G-G-C triplexes, whereas Zn++ prevents its formation, both at neutral and acidic pH. The poly(dC) . poly(dG) complex with Zn++ is of the B form, but its X-ray diffraction pattern shows an unusual intensity distribution. This is probably due to the fact that counterions occupy defined positions on the helix. The A form has not been observed. With poly[d(A-G)].poly [d(C-T)] a different triple helical structure is formed, both with Zn++ and Mg++. Direct, X-ray diffraction evidence for these triple helices is provided here for the first time.

DNA-RNA hybrid secondary structures

DNA-RNA and DNA-DNA duplexes are even more polymorphic than observed previously. DNA-RNA hybrids can have secondary structures like A-DNA or A-RNA, but double helices of the synthetic DNA-RNA hybrids poly(dA) X poly(rU) and poly(dI) X poly(rC), respectively, form 11-fold and 10-fold double-helical structures in which the two chains have quite different conformations. Extensive X-ray fiber diffraction analyses show that in both structures the DNA chains have C-2'-endo-puckered furanose rings, while the anti-parallel RNA chains have C-3'-endo-puckered rings. The bidirectional properties of such duplexes may be important in the transfer of biological information from nucleic acids.

New wrinkles on polynucleotide duplexes

Most fibrous polynucleotides of general sequence exhibit secondary structures that are described adequately by regular helices with a repeated motif of only one nucleotide. Such helices exploit the fact that A:T, T:A, G:C, and C:G pairs are essentially isomorphous and have dyadically-related glycosylic bonds. Polynucleotides with regularly repeated base-sequences sometimes assume secondary structures with larger repeated motifs which reflect these base-sequences. The dinucleotide units of the Z-like forms of poly d(As4T):poly d(As4T), poly d(AC):poly d(GT) and poly d(GC):poly d(GC) are dramatic instances of this phenomenon. The wrinkled B and D forms of poly d(GC):poly d(GC) and poly d(AT):poly d(AT) are just as significant but more subtle examples. It is possible also to trap more exotic secondary structures in which the molecular asymmetric unit is even larger. There is, for example, a tetragonal form of poly d(AT):poly d(AT) which has unit cell dimensions a = b = 1.71nm, c = 7.40nm, gamma = 90 degrees. The c dimension corresponds to the pitch of a molecular helix which accommodates 24 successive nucleotide pairs arranged as a 4(3) helix of hexanucleotide duplexes. The great variety of nucleotide conformations which occur in these large asymmetric units has prompted us to describe them as pleiomeric, a term used in botany to describe whorls having more than the usual number of structures. Pleiomeric DNAs need not contain nucleotide conformations that are very different from one another. On the other hand, DNAs carrying nucleotides of very different conformation must be pleiomeric. This is because 4 nucleotides of different conformation are needed to join patches of secondary structure which are as different as A or B or Z. Differences in nucleotide structures may occur also between chains rather than within chains. In poly d(A):poly d(T), the purine nucleotides all contain C3'-endo furanose rings and the pyrimidine nucleotides C2'-endo rings. Analogous heteronomous structures may exist in DNA-RNA hybrids although these duplexes are also found to have symmetrical A-type conformations.

Hydrogen exchange kinetics of nucleic acids. Double and triple helices with Hoogsteen-type basepairs

The kinetics of hydrogen-tritium exchange reaction have been followed by a Sephadex technique of a double-helical poly(ribo-2-methylthio-adenylic acid) . poly(ribouridylic acid) complex with the Hoogsteen-type basepair. Only one hydrogen in every 2-methylthio-adenine . uracil basepair has been found to exchange at a measurably slow rate, 0.023 s-1 (at 0 degrees C), which is, however, much greater than that for a double-helix with the Watson-Crick type A . U pair. The kinetics of hydrogen-tritium exchange were also examined by triple-helical poly(rU) . poly(rA) . poly(rU) which involves both the Watson-Crick and Hoogsteen basepairings. Here, three hydrogens in every U . A. U base triplet have been found to exchange at a relatively slow rate, 0.0116 s-1 (at 0 degrees C). The kinetics of hydrogen-deuterium exchange reactions of these polynucleotide helices have also been followed by a stopped-flow ultraviolet absorption spectrophotometry at various temperatures. On the basis of these experimental results, the mechanism of the hydrogen exchange reactions in these helical polynucleotides was discussed. In the triple helix, the rate-determining process of the slow exchange of the three (one uracil-imide and two adenine-amino) hydrogens is considered to be the opening of the Watson-Crick part of the U. A. U triplet. This opening is considered to take place only after the opening of the Hoogsteen part of the triplet.

Poly(U)-directed peptide-bond formation from the 2'(3')-glycyl esters of adenosine derivatives

The self-condensation of 2'(3')-O-glycyl esters of adenosine, adenosine-5'-(O-methylphosphate) and P1, P2-diadenosine-5'-pyrophosphate in 6.2 mM solutions at pH 8.0 and -5 degrees C in the presence of 12.5 mM poly(U) yields approximately 3 times as much diketopiperazine as reactions without poly(U). As the concentration of 2'(3')-O-(glycyl)-P1, P2-diadenosine-5'-pyrophosphate is decreased from 6.2 mM to 1.5 mM the yield of diketopiperazine in the presence of poly(U) decreases slightly from 6.6% to 5.2%, whereas, in the absence of poly(U) the yield of diketopiperazine decreases substantially from 2.4% to 0.75%. The enhanced yield of diketopiperazine that is attributed to the template action of poly(U) is temperature dependent and is observed only at temperatures below 10 degrees C (5 degrees C to -5 degrees C) for 6.2 mM 2'(3')-O-(glycyl)-adenosine-5'-(O-methylphosphate) and below 23 degrees C (15 degrees C to -5 degrees C) for 6.2 mM 2'(3')-O-(glycyl)-P1, P2-diadenosine-5'-pyrophosphate. The absence of a template effect at high temperatures is attributed to the melting of the organized helices. The hydrolysis half-lives at pH 8.0 and -5 degrees C of 2'(3')-O-(glycyl)-adenosine, 2'(3')-O-(glycyl)-adenosine-5'-(O-methylphosphate), 2'(3')-O-(glycyl)-P1, P2-diadenosine-5'-pyrophosphate, and 5'-O-(glycyl)-adenosine in the presence of poly(U) are substantially larger than their half-lives in the absence of poly(U). The condensation of 2'(3')-O-(glycyl)-adenosine yields 5% of 5'-O-(glycyl)-adenosine in the presence of poly(U) compared to 0.7% in the absence of poly(U).

The interaction of 2,6,8-triaminopurine with poly(uridylic acid)

Equilibrium dialysis measurements have shown that poly(uridylic acid) binds 2,6,8-triaminopurine in a strongly cooperative manner to form a stable 2 : 1 complex at pH 7.8, 0.15 M Na+. The thermal dissociation of the complex has been characterized by ultraviolet absorbance versus temperature profiles. From the variation of Tm with the concentration of uncomplexed triaminopurine at this temperature, the partial molar enthalpy and entropy of formation of the complex have been calculated as --87 (+/- 2) kJ/mol of triaminopurine and --236 (+/- 7) J/mol of triaminopurine per K, respectively. In terms of Tm, the complex is approximately 4 degrees C more stable than the corresponding 2 : 1 complex of poly(U) with 2-aminoadenine. This stabilization is attributed to the existence of an additional hydrogen-bonding interaction, in the poly(U)-triaminopurine complex, between the 8-amino group of 2,6,8-triaminopurine and O(2) of the uracil moiety which is base paired with it in Hoogsteen fashion.

Polynucleotide duplexes based on poly(7-deazaadenylic acid)

In order to find a poly(A)-poly(U) analog which could not form a triple-stranded complex and which would have a sufficiently high thermal stability to survive under physiological conditions, the interaction of poly(7-deazaadenylic acid) (poly(c-7A)) with modified polyuridylic acids was examined. Mixing curves constructed by the method of continuous variation, isosbestic points and thermal melting profiles proved that poly(c-7A) formed only 1:1 complex with polyribothymidylic acid and poly(5-bromouridylic acid) (Tm values of 50 and 72 degrees C respectively, in 0.15 M NaCl, 0.01 M KH2 PO4, 0.001 M MgCl2, pH7). In addition poly(c-7A) formed a 1:1 complex with poly(I) (Tm equals 22 degrees C in 0.46 M salt, pH 7), and presumed duplexes were observed in the interaction of poly(c-7A) with poly(dT), poly(2'-azido-2'-deoxyuridylic acid) and poly(2'-O-methyluridylic acid) (Tm values of 35, 32 and 41 degrees C respectively, in 0.10 M NaCl, pH7).