The structure of triple helical poly(U).poly(A).poly(U) studied by Raman spectroscopy

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U).poly(A).poly(U) triple helix. We compared the Raman spectra of poly(U).poly(A).poly(U) in H2O and D2O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A).poly(U). The presence of a Raman band at 863 cm-1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3' endo; that of the second poly(U) chain may be C2' endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A).poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.     

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.     

Free energy of the binding of uridylic acid oligomers with double stranded poly(A) x 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).     

Antisera to poly(A)-poly(U)-poly(I) contain antibody subpopulations specific for different aspects of the triple helix.

Rabbit antibodies to the triple-helical polynucleotide poly(A)-poly(U)-poly(I) were fractionated into three major antibody populations, each recognizing a different conformational feature of the triple-helical immunogen. Two distinct populations were purified from precipitates made with poly(A)-poly(U)-poly(U) and poly(A)-poly(I)-poly(I). The former reacted with double-stranded poly(A)-poly(U) or poly(I)-poly(C), and similar populations could be purified with either double-stranded form. The second population recognized the poly(A)-poly(I) region of the triple helix, and the third required all three strands for reactivity. These immunochemical studies suggest that the poly(A) and poly(U) have the same orientation in the triple-helicical poly(A)-poly(U)-poly(I) as in the double-helical poly(A)-poly(U), in which they have Watson-Crick base pairing.     

Local effects of partial adenine-N1-oxidation on poly A-poly U and poly A-2 poly U helix conformations

We prepared helices with noncomplementary bases by N1-oxidation of poly A, followed by reaction with poly U. Mixing curves indicate that doubly and triply helical structures form, with only the unmodified adenines involved in base pair formation. Circular dichroism spectra were examined particularly at the absorbance maximum of the adenine N1-oxide (A*). In the single strand poly (A,A*), there is a relatively strong pair of positive and negative CD bands from the A*. These are greatly reduced in the double helix, and abolished in the triple helix. We conclude that A* stacks in a conventional manner with A in the single strand, but is rotated out of the double and triple helix. In the double helix the A* probably maintains a preferred orientation with respect to the helix, but rotates randomly in the triple helix.     

Poly(rA) binds poly(rG).poly(rC) to form a triple helix.

Poly(rA) binds poly(rG).poly(rC) to form a triple helix. Evidence for this structure includes ultraviolet absorbance mixing curves and melting curves, and circular dichroism spectroscopy. The formation of the triple helix depends on the length of the poly(rC) strand. Triple helix forms when the average length is around 100 nucleotides but does not form when the average length is about 500 nucleotides.     

Theory of melting of the triple helix poly (A + 2U) for a 1 : 2 mixture of Poly A to Poly U

The Zimm-Bragg theory is extended to treat the melting of the triple helix poly (A + 2U) for a solution with a 1 : 2 mole ratio of poly A to poly U. Only the case for long chains is considered. For a given set of parameters the theory predicts the fraction of segments in the triple helix, double helix, and random coil states as a function of temperature. Four nucleation parameters are introduced to describe the two order–disorder transitions (poly (A + 2U) ? poly A + 2 poly U and poly (A + U) ? poly A + poly U) and the single order–order transition (poly (A + 2U) ? poly (A + U) + poly U). A relation between the nucleation parameters is obtained which reduces the number of independent parameters to three. A method for determining these parameters from experiment is presented. From the previously published data of Blake, Massoulié and Fresco⁸ for [Na⁺] = 0.04, we find σ_T = 6.0 × 10^?4, σ_D = 1.0 × 10^?3, and σσ* = 1.5 × 10^?3. σ_T and σ_D are the nucleation parameters for nucleating a triple helix and double helix, respectively, from a random coil region. σσ* is the nucleation parameter for nucleating a triple helix from a double helix and a single strand. Melting curves are generated from the theory and compared with the experimental melting curves.     

Base-pair opening and closing reactions in the double helix. A stopped-flow hydrogen exchange study in poly(rA).poly(rU).

The hydrogen-deuterium exchange of AMP, uridine, poly(rA), and poly(rA) · poly(rU) was investigated by a spectral difference method using stopped-flow spectrophotometry. Proton exchange rates were measured as a function of pH, added catalysts, temperature and salt concentration. The results confirm and extend previous conclusions on the H-exchange chemistry of the bases, on the large equilibrium opening of the double helix, and on its slow opening and closing rates, but an alternative conformation for the major open state is considered. Two H-exchange rate classes are found in poly(rA) · poly(rU). The slower class represents the two exocyclic amino protons of A which exchange through a pre-equilibrium opening mechanism, therefore revealing the fraction of time the helix is open. Base-pairs are open 5% of the time at 25 °C. The faster class is assigned to the U-N-3 H proton, the rate of which is limited by helix opening. Both opening and reclosing of the duplex are slow, 2 s^?1 and 40 s^?1, respectively, at 25 °C. Thermodynamic parameters for the equilibrium helix opening and for the rate of opening were determined. These properties may be consistent with a simple opening involving swinging out of the U base while retaining A more or less stacked within the duplex. The results demonstrate that no faster or more populated helix-open state occurs (when structure is stable). It appears that, unlike opening—closing reactions at a helix end or a helix-coil boundary, internal base opening and closing are innately slow. One implication of this is that any chemical or biological process requiring access to sequences in the interior of a closed stable DNA duplex may be constrained to proceed only on a time scale of seconds, and not in milliseconds or microseconds.     

Phosphorus-31 nuclear magnetic resonance of double- and triple-helical nucleic acids. Phosphorus-31 chemical shifts as a probe of phosphorus-oxygen ester bond torsional angles

The temperature dependence to the 31P NMR spectra of poly[d(GC)] . poly [d(GC)],d(GC)4, phenylalanine tRNA (yeast) and mixtures of poly(A) + oligo(U) is presented. The 31P NMR spectra of mixtures of complementary RNA and of the poly d(GC) self-complementary DNA provide torsional information on the phosphate ester conformation in the double, triple, and "Z" helix. The increasing downfield shift with temperature of the single-strand nucleic acids provides a measure of the change in the phosphate ester conformation in the single helix to coil conversion. A separate upfield peak (20-60% of the total phosphates) is observed at lower temperatures in the oligo(U) . poly(A) mixtures which is assigned to the double helix/triple helix. Proton NMR and UV spectra confirm the presence of the multistrand forms. The 31P chemical shift for the double helix/triple helix is 0.2-0.5 ppm upfield from the chemical shift for the single helix which in turn is 1.0 ppm upfield from the chemical shift for the random coil conformation.     

The Structure of Triple Helical Poly(U)·Poly(A)·Poly(U) Studied by Raman Spectroscopy

Abstract

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U)·poly(A) ·poly(U) triple helix. We compared the Raman spectra of poly(U)·poly(A)·poly(U) in H₂O and D₂O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A)·poly(U). The presence of a Raman band at 863 cm^?1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3′ endo; that of the second poly(U) chain may be C2′ endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A)·poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.     

Model building of DNA/RNA triple helix containing L-deoxyadenosine.

A three-dimensional model of DNA/RNA triple helix that contains a poly(L-deoxyadenosine) (L-dA) chain is proposed based on computer-assisted model building and energy calculations. The model building was performed by a new method that systematically searches possible conformations of nucleotide units in the helical chains. Two possible orientations of sugar-phosphate chains, in which two homopyrimidine strands are parallel or antiparallel with each other, were considered in the systematic search. Several possible base-pairing models, in which there are one Watson-Crick base pair and one other base pair, were also considered. Many possible models selected by the systematic search were further refined through molecular mechanics calculation incorporating a helical boundary condition. The preferred model, which was selected on the basis of potential energy, was the one with Watson-Crick and Hoogsteen base pairs and with its two polypyrimidine chains in the antiparallel orientation. The model can explain the experimental observation that poly(L-dA) forms a stable triple helix with poly(uridylic acid) (U) but not with poly(deoxythymidylic acid) (dT).     

Properties of unprimed poly(A)-poly(U) synthesis by Caulobacter crescentus RNA polymerase.

Some properties of unprimed poly(A)-poly(U) synthesis by DNA-dependent RNA polymerase from Caulobacter crescentus were examined. The reaction required ATP and UTP as substrates and manganese as a divalent cation. Rifampicin completely inhibited the reaction at a concentration of 1 micron/ml, and the enzyme catalyzed the polymer synthesis well regardless of the presence of GTP, CTP or both. The chain length of the poly(A)-poly(U) synthesized was about one hundred base pairs, as estimated from a sedimentation velocity and the molar ratio of [3H]AMP to [gamma-32P]ATP incorporated into the poly(A)-poly(U). The reaction was dependent on the square of the enzyme concentration and the enzyme dimers formed complexes with poly(A)-poly(U) during the reaction.     

Protonated polynucleotide structures. 18. Interaction of oligocytidylates with poly (G).

The faculty for and degree of oligo(C)-poly(G) interaction is described as an essentially chain length - sensitive phenomenon. At neutral pH under suitable experimental conditions, oligocytidylates of chain length greater than four associate with poly(G) to form double-stranded structures, as does poly(C). The extent of complex formation increases with degree of polymerization. The complex at acid pH is shown to be triple-stranded, of stoicheometry 2C/1G. The observation of a 2G/1C artifact is discussed.     

Location of oligo(uridylic acid) sequences within messenger ribonucleic acid molecules of HeLa cells

A significant fraction of the polyadenylated mRNAs of HeLa cells contain an oligo(uridylic acid) [oligo(U)] sequence of 15-30 nucleotides. Several different experimental approaches were used to determine if these oligo(U)'s occupied similar sites within all mRNAs. In one approach, poly(adenylic acid)-containing mRNAs [poly(A+) mRNAs] averaging 2800 nucleotides in length were reduced to an average size of 500 nucleotides by controlled alkaline hydrolysis. Over 20% of the oligo(U)-containing fragments isolated from the hydrolysate retained a poly(A) sequence, showing that oligo(U)'s were not exclusively located near 5' ends of mRNA although 20% were apparently close to 3' ends. To confirm these observations, oligo(U)-containing mRNA [oligo(U+) mRNA] was exposed to the 3'-exonucleolytic activity of polynucleotide phosphorylase to produce fragments containing the 5' regions of mRNA. Each of a set of fragments of decreasing length generated by increased times of exposure of the mRNAs to the enzyme was found to have about the same oligo(U) content, including the shortest that averaged 550 nucleotides. These data not only eliminated an exclusive location for oligo(U) in either 3' or 5' ends of mRNA but also suggested that oligo(U)'s might be close to the 5' ends of some mRNAs. To verify this last observation, periodate-oxidized poly(A+) mRNA was labeled at the 5' caps and at 3'-adenosine residues by sodium [3H]borohydride reduction before it was nicked 3-5 times with alkali to produce 5' and 3' end-labeled pieces that could be separated with oligo(thymidylic acid)-cellulose.(ABSTRACT TRUNCATED AT 250 WORDS)     

Observations on the kinetics of action of polyspermine-ribonuclease on poly(A).poly(U).

Starting from the observation that double-stranded ribonucleic acids are hydrolyzed more rapidly by bovine pancreatic ribonuclease that has been cross-linked to polyspermine, we have made an initial examination of the kinetics of the process. The addition of eight residues of the polyamine serves to strengthen the binding to poly(A).poly(U) 100-fold (Km changes from 2.7 . 10(-4) to 2.7 . 10(-6) M in total U) and to increase V for hydrolysis of the susceptible poly(U) strand from 2.5 to 16.2 delta A250 . min-1 per mg enzyme. There is evidence for inhibition by the RNAase-resistant poly(A) tracts in the substrate; free poly(A) shows a Ki of about 8 . 10(-6) M in total A.     

Cooperative binding of a platinum metallointercalation reagent to poly(A).poly(U).

The cationic complex (2-hydroxyethanethiolato)(2,2',2'-terpyridine)platinum(II), [(terpy)Pt(HET)]+, binds cooperatively to poly(A).poly(U) by intercalation. The melting temperature of poly(A).poly(U) in low-salt buffer is increased by 6 degrees C in the presence of [(terpy)Pt(HET)]+, indicating stabilization of the duplex structure by the bound platinum reagent. Viscosity measurements provide evidence for comparable lengthening of the polynucleotide in the presence of [(terpy)Pt(HET)]+ and the intercalating dye, ethidium bromide. Scatchard plots of the binding of [(terpy)Pt(HET)]+ to poly(A).poly(U) and poly(I).poly(C), determined through ultracentrifugation pelleting methods, show large positive curvature, reflecting the strong cooperativity associated with the platinum complex-RNA interaction. The characteristics of the binding isotherms are interpreted in terms of a model where cooperative pair units of [(terpy)Pt(HET)]+ intercalate into the double-stranded polymer. At saturation, two platinum molecules are bound for every three base pairs. This stoichiometry may be compared with the nearest-neighbor-exclusion binding observed previously in the interaction of [(terpy)Pt(HET)]+ and the ethidium cation with DNA, in which one intercalator occupies every other interbase-pair site at saturation. The striking differences observed in the interaction of [(terpy)Pt(HET)]+ with DNA and RNA suggest that drug recognition is sensitive to the constraints imposed by nucleic acid secondary structure.     

A calorimetric study of the triple helix formation: interaction of poly(C) - guanosine - protonated poly(C).]

The triple helix formation of poly(C) - guanosine - poly(C+) was investigated by the help of an LKB scanning micro-calorimeter. The existence of the triple helix could also be shown by recording the melting curves. The ultraviolet absorption at different wave lengths namely 275 nm, 260 nm, and 245 nm was plotted as a function of the temperature. Furthermore formation of the triple helix was shown by plotting the ultraviolet absorption at 245 nm during the increasing addition of guanosine solution to a fixed amount of poly(C) in the solution. Finally the formation of the triple helix was demonstrated by plotting the ultraviolet absorption at 245 nm of a certain mixture of the components while the pH value of the solution was continuously lowered. All these methods show that the monomer interacts with the polymer double helix to form a triple helix. The calorimetric measurements show that the reaction enthalpy is concentration dependent. Above a threshold concentration a rapid increase of the reaction enthalpy is observed. This increase occurs in a very narrow concentration interval. Above this interval a final value of the reaction enthalpy is reached. The amount of the reaction enthalpy for the interaction of guanosine with poly(C) - poly(C+) double helix is 5.5 Kcal (mol base triplet)-1.     

Characterization of product RNAs synthesized in vitro by poliovirus RNA polymerase purified by chromatography on hydroxylapatite or poly(U) Sepharose.

The size of the product RNA synthesized by the poliovirus RNA polymerase and host factor was significantly affected by the type of column chromatography used to purify the polymerase. Dimer length product RNA was synthesized by the polymerase purified by chromatography on hydroxylapatite. This contrasted with the monomer length product RNA synthesized by the polymerase purified by chromatography on poly(U) Sepharose. The poly(U) Sepharose-purified polymerase was shown to contain oligo(U) that functioned as a primer. The addition of host factor to reactions containing the poly(U) Sepharose-purified polymerase significantly increased the synthesis of monomer length product RNA, in agreement with previous studies. This product RNA, however, did not immunoprecipitate with anti-VPg antibody and thus was not linked to VPg or a VPg-related protein. Thus, it was concluded that the synthesis of monomer length product RNA by the poly(U) Sepharose-purified polymerase and host factor was caused by oligo(U) priming rather than VPg priming.     

The thermodynamic contribution of the 5-methyl group of thymine in the two- and three-stranded complexes formed by poly(dU) and poly(dT) with poly(dA)

To assess the thermodynamic contribution of the 5-methyl group of thymine, we have studied the two-stranded helical complexes poly(dA).poly(dU) and poly(dA).poly(dT) and the three-stranded complexes--poly(dA).2poly(dU), poly(dA).poly(dT).poly(dU) and poly(dA).2poly(dT)--by differential scanning calorimetry, and uv optical melting experiments. The thermodynamic quantities associated with the 3 --> 2, 2 --> 1, and 3 --> 1 melting transitions are found to vary with salt concentration and temperature in a more complex manner than commonly believed. The transition temperatures, T(m), are generally not linear in the logarithm of concentration or activity of NaCl. The change in enthalpy and in entropy upon melting varies with salt concentration and temperature, and a change in heat capacity accompanies each transition. The poly(dA).2poly(dU) triple helix is markedly different from poly(dA).2poly(dT) in both its CD spectrum and thermodynamic behavior, while the poly(dA).poly(dT).poly(dU) triple helix resembles poly(dA).2poly(dT) in these properties. In comparing poly(dA).2poly(dT) with either the poly(dA).poly(dT).poly(dU) or the poly(dA).2poly(dU) triplexes, the substitution of thymine for uracil in the third strand results in an enhancement of stability against the 3 --> 2 dissociation of deltadeltaG degrees = -135 +/- 85 cal (mol A)(-1) at 37 degrees C. This represents a doubling of the absolute stability toward dissociation compared to the triplexes with poly(dU) as the third strand. The poly (dA).poly (dT) duplex is more stable than poly(dA).poly(dU) by deltadeltaG degrees = -350 +/- 60 cal (mol base pair)(-1) at 37 degrees C. Poly(dA).poly(dT) has 50% greater stability than poly(dA).poly(dU) as a result of the dT for dU substitution in the duplex.