Halogenated nucleic acids: effects of 5-fluorouracil on the conformation and properties of a polyribonucleotide and its constituents

The conformational properties of 5-fluorouracil derivatives are compared to uracil derivatives. FUrd, 5′-FUMP, and poly(FU) are studied as a function of pH and temperature by ¹⁹F- and ¹H-nmr spectroscopy, and the corresponding uracil derivatives by ¹H-nmr spectroscopy. FUrd exhibits no significant conformational changes with solution pH (5–10). In contrast, at low pH (6–7) 5′-FUMP and 5′-UMP show similar conformational features, while at high pH (9) 5′-FUMP shows significant conformational alterations. Also, poly(U) and poly(FU) are conformationally similar at low pH, but increasing pH induces changes in poly(FU). These changes are observed in the backbone [γ(C4′-C5′)], furanose, and furanose-base conformations. The apparent pK_a of N3-H ionization of the FUra base is determined by ¹H- and ¹⁹F-nmr to range from 7.5 to 8.2 [FUrd < 5′-FUMP < 5′-FUDP < poly(FU)]. These observations are interpreted as a result of electrostatic interactions generated between the ionized phosphate group and the negatively charged base moiety as the pH is raised. The interaction properties of poly(FU) with ApA are studied by ¹H- and ¹⁹F-nmr spectroscopy, and these properties compared to those published for poly(U). Poly(FU) forms a complex with ApA inducing upfield ¹H-shifts in both components, and downfield ¹⁹F- shifts in poly(FU). The base stoichiometry of the complex for poly(U)·ApA is 2U:1A at various U/A ratios. In contrast, the base stoichiometry of the poly(FU)·ApA complex appears to be dependent on the FU/A ratio. At high FU/A ratio, the complex is 2FU:1A, and as the FU/A ratio approaches unity the complex becomes 1FU:1A.     

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.     

Three-stranded helix-coil equilibrium in polyuridylic acid-adenosine complex

Interaction of poly U (polyuridylic acid) and adenosine is studied by following the changes in ultraviolet absorbance in the wavelength region near the isochromic wave-length for the complex formation. The interaction is studied as a function of temperature, concentration of adenosine, and ionic strength, while the concentration of poly U was held constant. It is confirmed that only the three-stranded complex with the stoichiometry 1A to 2U is formed and that it dissociates directly into free poly U and adenosine. No discontinuity of any kind was apparent in the melting curves, and poly U was found to possess no ordered structure above 10°C under the conditions used. The results were, therefore, analyzed in terms of an exact helix–coil equilibrium theory using the mismatching model, i.e., assuming that either completely formed base triplet or completely free unbonded bases only exist, and that the two sections of the polymer chains forming closed loops need not contain the same number of unbonded bases. Self-association of free adenosine was taken into consideration. (Base triplet is analog of base pair for a three-stranded helical complex. It refers to a unit of three coplanar bases, in this case two uracils and one adenine, hydrogen bonded to one another to form a triplet. Such triplets may stack over one another along the helical axis, and when they are so stacked the bases of two triplets next to each other may have stacking interactions between them.) The values for enthalpy and entropy changes, both per mole of base triplets, were obtained for the following processes at neutral pH and moderate to high salt concentrations. (1) Growfh: Binding of one adenosine molecule to two uracil residues (one from each poly U strand) to form a base triplet next to an already formed base triplet with which it has stacking interactions, a process that involves both hydrogen bonding and base stacking interactions, ΔH_s, = ?19 ± 2 kcal, ΔS_s = ?55 ± 6 clausius; (2) Initiation: Binding of one adenosine molecule to two uracil residues (one from each poly U strand) to form an isolated base triplet, a process that involves only hydrogen bonding interactions, ΔH_b* = 4.5 ± 2 kcal, ΔS_b* = 6.6 ± 3 clausius; and (3)Interruption: Unstacking of two stacked base triplets initially next to each other by formation of an interruption (viz. a closed loop) between them, a process that involves only base stacking interactions, ΔH_b = 23.5 ± 3 kcal, ΔS_b = 61.6 ± 7 clausius, where the entropy changes include contributions other than the configurational entropy of closed loops. The discrepancy between our results and the calorimetric ΔH_s of ?13 kcal is attributed to (i) the possible effects of salt arid polymer on the self-association of free adenosine, (ii) the uncertainty in the value of the parameter for the probability of ring closure, and (iii) the contributions due to the partial molal enthalpy of the solvent and the unstacking of any poly U structure to the calorimetric enthalpy.     

Sequence and conformational effects on imino proton exchange in A.T- and A.U-containing DNA and RNA duplexes

¹H-nmr relaxation has been used to study the effect of sequence and conformation on imino proton exchange in adenine–thymine (A · T) and adenine–uracil (A · U) containing DNA and RNA duplexes. At low temperature, relaxation is caused by dipolar interactions between the imino and the adenine amino and AH2 protons, and at higher temperature, by exchange with the solvent protons. Although room temperature exchange rates vary between 3 and 12s^?1, the exchange activation energies (E_α) are insensitive to changes in the duplex sequence (alternating vs homopolymer duplexes), the conformation (B-form DNA vs A-form RNA), and the identity of the pyrimidine base (thymine vs uracil). The average value of the activation energy for the five duplexes studied, poly[d(A-T)], poly[d(A) · d(T)], poly[d(A-U)], Poly[d(A) · d(U)], and poly[r(A) · r(U)], was 16.8 ± 1.3 kcal/mol. In addition, we find that the average E_α for the A.T base pairs in a 43-base-pair restriction fragment is 16.4 ± 1.0 kcal/mol. This result is to be contrasted with the observation that the E_α of cytosine-containing duplexes depends on the sequence, conformation, and substituent groups on the purine and pyrimidine bases. Taken together, the data indicate that there is a common low-energy pathway for the escape of the thymine (uracil) imino protons from the double helix. The absolute values of the exchange rates in the simple sequence polymers are typically 3–10 times faster than in DNAs containing both A · T and G · C base pairs.     

The reaction of 14C-labelled platinum ethylenediamine dichloride with adenine compounds and DNA

Various derivatives of adenine have been studied with regard to their rate of reaction with ¹⁴C-labelled platinum ethylenediamine dichloride, Pt(¹⁴C-en)Cl₂. The reactivities have been calculated from the “rate of disappearance” of Pt(¹⁴C-en)Cl₂ using chromatographic separation of reactants and products.Adenine and adenosine react very slowly at 37° whereas other adenine derivatives react much more readily in the order: poly A > AMP > ApA > poly d(AT). From the numerical values of the rate constants it is concluded that the presence of a phosphate group increases the reaction rate considerably. This is partly the explanation of the rapid reaction of poly A which possesses terminal phosphate groups. However adjacent adenine moieties such as those in polyadenylic acid (poly A) and adenosyl-3′5′-adenosine (ApA) may also react by another mechanism which involves the 6-NH₂ groups.The energies of activation of the second order reaction with platinum ethylenediamine dichloride (PtenCl₂) are 12.9, 18.8, 19.0 kcal/mole for poly A, AMP and ApA respectively.In DNA, no free phosphate groups are present, and the occurrence of adjacent adenines will be low. The reaction of PtenCl₂ with DNA seems to involve a rapid attack on deoxyguanosine (GdR) and a slow reaction with deoxyadenosine (AdR) and deoxycytidine (CdR).     

Proton magnetic resonance study of the binding of purine to polyuridylic acid

The interaction of unsubstituted purine with polyuridylic acid in D₂O solution at neutral pD has been studied by high resolution proton magnetic resonance spectroscopy. The poly U proton resonances were shifted to higher fields by the added purine, indicating that purine binds to the uracil bases of the polymer by base stacking. Severe broadening of the purine proton resonances was also observed, providing strong evidence for the intercalation of purine between adjacent uracil bases of the polymer. The line widths of the poly U proton resonances were not noticeably broadened in the presence of purine; thus, the binding of purine to poly U does not result in a more rigid or ordered structure for the polymer.     

Proton magnetic resonance study of complex formation between N6-methyladenosine and polyuridylic acid

The interaction between N₆-methyladenosine and polyuridylic acid in D₂O solution at neutral pD has been studied as a function of temperature and N₆-methyladenosine concentration by proton magnetic resonance spectroscopy. A rigid double-stranded 1:1 complex is formed below ～10°C, involving hydrogen-bonded N₆-methyladenine:uracil base-pairing and stacking of the adenine bases. This complex is less stable than the 1:2 complex formed between adenosine and polyU, and involves a more rapid exchange of the monomer between free and polymer-bound environments.     

First-principles study of interaction of serine with nucleobases of DNA and RNA

The nature of interaction between serine—a vital molecule for cancer cell proliferation and nucleic acid bases—adenine (A), guanine (G), cytosine (C), thymine (T), and uracil (U) is investigated within the framework of Møller–Plesset perturbation theory (MP2) and density functional theory (DFT). To quantify the interaction strength between serine and nucleobases, the corresponding binding energies were computed, showing energetic ordering such that G?>?C?>?T?>?A?>?U. This shows that the interaction energy of serine with guanine is the highest, while with uracil it is the lowest. The amount of charge transferred is the lowest in case of the serine-guanine complex and highest in case of the serine-uracil complex. The results show the serine-guanine complex to be more stable and to have a salt bridge structure involving the -COOH group. Theoretical analysis based on MP2 and DFT shows that the interaction between the serine and nucleobases is mainly determined by hydrogen bonding.     

Purine and pyrimidine metabolism in cultured white spruce (Picea glauca) cells: Metabolic fate of 14C-labeled precursors and activity of key enzymes

In order to examine the biosynthesis, interconversion, and degradation of purine and pyrimidine nucleotides in white spruce cells, radiolabeled adenine, adenosine, inosine, uracil, uridine, and orotic acid were supplied exogenously to the cells and the overall metabolism of these compounds was monitored. [8‐¹⁴C]adenine and [8‐¹⁴C]adenosine were metabolized to adenylates and part of the adenylates were converted to guanylates and incorporated into both adenine and guanine bases of nucleic acids. A small amount of [8‐¹⁴C]inosine was converted into nucleotides and incorporated into both adenine and guanine bases of nucleic acids. High adenosine kinase and adenine phosphoribosyltransferase activities in the extract suggested that adenosine and adenine were converted to AMP by these enzymes. No adenosine nucleosidase activity was detected. Inosine was apparently converted to AMP by inosine kinase and/or a non‐specific nucleoside phosphotransferase. The radioactivity of [8‐¹⁴C]adenosine, [8‐¹⁴C]adenine, and [8‐¹⁴C]inosine was also detected in ureide, especially allantoic acid, and CO₂. Among these 3 precursors, the radioactivity from [8‐¹⁴C]inosine was predominantly incorporated into CO₂. These results suggest the operation of a conventional degradation pathway. Both [2‐¹⁴C]uracil and [2‐¹⁴C]uridine were converted to uridine nucleotides and incorporated into uracil and cytosine bases of nucleic acids. The salvage enzymes, uridine kinase and uracil phosphoribosyltransferase, were detected in white spruce extracts. [6‐¹⁴C]orotic acid, an intermediate of the de novo pyrimidine biosynthesis, was efficiently converted into uridine nucleotides and also incorporated into uracil and cytosine bases of nucleic acids. High activity of orotate phosphoribosyltransferase was observed in the extracts. A large proportion of radioactivity from [2‐¹⁴C]uracil was recovered as CO₂ and β‐ureidopropionate. Thus, a reductive pathway of uracil degradation is functional in these cells. Therefore, white spruce cells in culture demonstrate both the de novo and salvage pathways of purine and pyrimidine metabolism, as well as some degradation of the substrates into CO₂.     

The adsorption of nucleotides and polynucleotides on montmorillonite clay

The binding of adenine derivatives to Na(+)-montmorillonite increases in the order 5'AMP, 3'-AMP, 5'ADP < adenosine < purine, adenine. With the exception of cytosine, cytosine derivatives bind less strongly than the corresponding adenine derivatives in the order 5'-CMP < cytidine < cytosine. There is little difference in the binding of uracil derivatives and these compounds bind less strongly than the corresponding adenine analogs. It is concluded that the adenine ring in adenine derivatives is protonated by the acidic montmorillonite surface and binding is a consequence of the electrostatic interaction between the protonated base and the negative charges on the surface of the montmorillonite. Different binding trends were observed with Cu(2+)-montmorillonite with AMP binding more strongly than adenosine and UMP binding more strongly than uridine. It is concluded that ligation to the Cu2+ is a major force in the binding of nucleotides to Cu(2+)-montmorillonite and are not readily washed from the clay. Factors contributing to the binding are discussed. Watson-Crick hydrogen bonding of 5'-AMP to poly(U) and 5'GMP to poly(C) was observed when the homopolymers are bound to the surface of the clay. No association of 5'-UMP to poly(U) bound to clay was detected. The possible role of montmorillonite clays in the prebiotic formation of RNA is discussed.     

Magnetic circular dichroism study on synthetic polynucleotides, bacteriophage structure, and DNA's

The MCD (magnetic circular dichroism) spectra of Ap, ApA, ApApA, poly A, Up, UpU, poly U and double-stranded poly A:U alternating copoly A–U and alternating deoxyribopoly A–T were measured with a Cary 61 spectropolarimeter fitted with a Varian superconducting magnet at a field strength of 50 Kgauss. The MCD spectra of T2 and T5 DNA at various stages of heal denaturation were measured as a function of hyperchromicity of the sample. MCD spectra of the intact and degraded T2 and T5 phages were used to study the degree of alteration of the DNA inside the phages versus the DNA in vitro. The results for the adenine polymers show that the main MCD bands, B_2u(271 nm), B_1u(252 nm), and E_1u(212 nm), show a decrease in specific magnitude as the length of the polymer is increased, reflecting the degree of stacking of the polymer. In contrast, the uridine series of polymers shows little change of the MCD bands, indicating that there is little interaction between the bases regardless of the length of the polymers. The MCD spectra of poly A:U, alternating poly r(A–U): (A–U), and alternating poly d(A–T):(A–T) show significant differences among themselves in the magnitude of the B_2u band and when compared with the sum of the spectrum for the poly A plus poly U. This may indicate the selective effect of hydrogen bonding on the B_2u band. Alternatively, the difference may be due to the absence of an n → π* transition in the double-stranded polymer. Measurements of denatured T2 and To DNA's show increases in all MCD bands. The T2 DNA internally packed in phage shows an increase of the B_2u and E_1ubands, the B_2u remaining unchanged. The internal T5 DNA shows an increase of the B_1u band only. Thus, the internal DNA structure is altered in a manner quite different from a simple denaturation caused by hydrogen bond breaking. Furthermore, different MCD bands indicate that different modes of DNA packing exist for T2 and T5 phages.     

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.     

Study of the interaction of polynucleotide chains with oligomers by means of chromatography. II. Effect of magnesium ions and noncomplementary bases on the stability of complexes

The interaction of the oligonucleotides ApA, ApApA, ApApC and ApApU with poly(U) and (Ip)₅I and (Ip)₆ with poly(C) has been studied by means of equilibrium gelfiltration through Sephadex.From sorption isotherms the free energies, energies and entropies of complexing have been computed for different concentrations of magnesium ions in the medium.The stoichiometric ratio of polymers to oligomers has been measured and found equal to 2 in the case of ApApA and ApApC. This shows that the cytidylic acid residue is included in the ternary complex. But in the case of ApApU the noncomplementary base is partly squeezed out of the complex.The stacking free energy of neighbouring oligomers has been found to be in the range 1000–3000 $\text{cal}\text{mole}$ depending on the conditions.The stoichimetric ratio has been found to be 1 in the case of poly(C): oligo(I), the stacking energy is equal to 1.2 $\text{kcal}\text{mole}$. The effect of magnesium is somewhat different in the case of double and triple helices and probably reflects the formation of coordination compounds with the nitrogen bases of nucleotides.     

Ultraviolet-induced 8,8-adenine dehydrodimers in oligo- and polynucleotides.

Characteristic fluorescence excitation and emission is induced by either acetone-sensitized 313 nm irradiation of mixtures of 8-bromoadenosine and adenosine or 254 nm irradiation of oligo- and polynucleotides containing adenine neighbors. The acetone-sensitized reaction involves cleavage of bromine from 8-bromoadenosine with activation of C-8, leading to formation of an 8,8-adenosine dehydrodimer. Comparable fluorescence properties arise in the unsensitized photoreaction of dApdA, pdApdA, ApA, poly(dA), poly(A), poly(dA.dT), and poly(dA.U). The previously unidentified adenine ultraviolet photoproduct described by Porschke has been isolated as several variants from solutions of pdApdA and poly(dA) irradiated at 254 nm. Based upon fluorescence spectra and mass spectra, these variants are shown to contain the 8,8-adenine dehydrodimer moiety.     

The structure of cytidilyl(2',5')adenosine when bound to pancreatic ribonuclease S

The three-dimensional structure of the RNase S complex with the synthetic dinucleoside monophosphate cytidilyl(2′,5′)adenosine(C₂,p₅,A) is determined using difference Fourier techniques at 2.0 Å resolution in conjunction with computer graphic model-building and energy minimization. The latter has been carried out as a function of the rigid body parameters of the dinucleoside monophosphate and the dihedral angles of the nucleoside portion as well as of relevent amino acids in the active site of the enzyme.The bound dinucleoside monophosphate is found to assume an extended conformation, with the adenine and cytidine bases nearly perpendicular. The bases form specific hydrogen bonds with groups in the active site. Although the atoms involved in the recognition of the pyrimidine base by the enzyme are the same as in the pyrimidine bases of UMP, CMP and UpcA, the details of the binding are different. The adenosine moiety blocks most of the various positions that His119 occupies in the native enzyme and forces it into one well-defined position. One of the His119 ring protons is in contact with O(5′) (the leaving group), O(1′) of the adenine ribose and with a free phosphoryl oxygen. No strong charge contacts with the phosphate group are observed.We show how combining X-ray data with computer graphic model-building, electron density fitting and energy calculations leads to the model we propose and discuss in detail the enzyme-nucleic acid interactions.     

The alternating conformation of analogues of poly[d(AT)].

Synthetic DNAs were prepared containing 6-methyl adenine (m6A) in place of adenine and 5-ethyl uracil (Et5U) or 5-methoxymethyl uracil (Mm5U) in place of thymine. All three modifications destabilized duplex DNAs to varying degrees. The binding of ethidium was studied to analogues of poly[d(AT)]. There was no evidence of cooperative binding and the "neighbour exclusion rule" was obeyed in all cases although the binding constant to poly[d(m6AT)] was approximately 6 fold higher than to poly[d(AT)]. 31P NMR spectra were recorded in increasing concentrations of CsF. Poly[d(AEt5U)] showed two well-resolved signals separated by 0.55 ppm in 1 M CsF compared to 0.32 ppm for poly[d(AT)] under identical conditions. In contrast, poly[d(AMm5U)] and poly[d(m6AT)] showed two signals separated by 0.28 ppm and 0.15 ppm respectively, only when the concentration of CsF was raised to 2 M. The signals for poly[d(AT)] in 2 M CsF were better resolved and were separated by 0.41 ppm. These results suggest that minor modifications to the bases may have conformational effects which could be recognized by DNA-binding proteins.     

The isolation and characterisation of a new type of dimeric adenine photoproduct in UV-irradiated deoxyadenylates.

A new type of dimeric adenine photoproduct has been isolated from d(ApA) irradiated at 254 nm in neutral aqueous solution. It is formed in comparable amounts to another, quite distinct, adenine photoproduct first described by Pörschke (J. Am. Chem. Soc. (1973), 95, 8440-8446). Results from high resolution mass spectrometry and 1H NMR indicate that the new photoproduct comprises a mixture of two stereoisomers whose formation involves covalent coupling of the adenine bases in d(ApA) and concomitant incorporation of the elements of one molecule of water. The photoproduct is degraded specifically by acid to 4,6-diamino-5-guanidinopyrimidine (DGPY) whose identity has been confirmed by independent chemical synthesis. Formation of the new photoproduct in UV-irradiated d(pA)2 and poly(dA), but not poly(rA), has been demonstrated by assaying their acid hydrolysates for the presence of DGPY. The properties of the photoproduct are consistent with it being generated by the hydrolytic fission of an azetidine photoadduct in which the N(7) and C(8) atoms of the 5''-adenine in d(ApA) are linked respectively to the C(6) and C(5) positions of the 3''-adenine.     

The vibrational spectra and structure of poly(rA-rU)-poly(rA-rU)

Infrared and Raman spectra of aqueous poly(rA-rU)·poly(rA-rU), the double-helical complex containing strands of alternating riboadenylate and ribouridylate residues, display significant differences from one another and from corresponding spectra of poly(rA)·poly(rU), the double-helical complex of riboadenylate and ribouridylate homopolymers. Parallel studies on the copolymer and homopolymer complexes by cesium sulfate density gradient centrifugation, ultraviolet absorption spectroscopy, hydrogenion titration, 1-N oxidation of adenine residues by monoperphthalic acid and X-ray diffraction reveal, however, that the geometry of base pairing between adenine and uracil is closely similar in each complex and apparently of the Watson-Crick type. Therefore the differences observed between vibrational spectra of poly (rA-rU)·poly (rA-rU) and poly(rA)·poly(rU) are not due to different base-pairing schemes but may be attributed to differences in vibrational coupling between vertically stacked bases. Vibrational coupling may also account for the differences between infrared and Raman spectra of the same complex. Thus, the present results indicate that infrared and Raman frequencies of RNA in the region 1750–1550 cm^?1 should be dependent on the base sequence.     

Study of salt effects on adenosine–polyuridylic acid interaction

Complex formation between poly(U) and adenosine in solutions of salts that stabilize (Na₂SO₄), destabilize (NaClO₄), or have little effect on the water structure (NaCl), as well as the poly(U)·poly(A) interaction in NaClO₄, was studied by equilibrium dialysis and uv spectroscopy. At 3°C and neutral pH, Ado·2 poly(U) is formed in 1M NaCl and 0.33M Na₂SO₄. In NaClO₄ solutions under the same conditions, an Ado·poly(U) was found over the whole range of salt concentration investigated (10 mM?1M), which has not been previously observed under any conditions. The Ado-poly(U) was also found in a NaCl/NaClO₄ mixture, the transition from the triple- to the double-helical complex occurring within a narrow range of concentration of added NaClO₄. In the presence of 1M NaCl this transition is observed on adding as little as 10 mM NaClO₄, i.e., at a [ClO]/[Cl^?] ratio of about 1:100. However, when NaClO₄ is added to a 1M solution of the stabilizing salt Na₂SO₄, no transition occurs even at a [ClO]/[SO] ratio of 1:4. Investigation of melting curves and uv spectra has shown that in an equimolar mixture of the polynucleotides, only a double-helical poly(U)·poly(A) exists in 1M NaClO₄ at low temperatures; this also holds for 1M NaCl. This changes to a triple-helical 2 poly(U)·poly(A) and then dissociates as the temperature increases. At low temperatures and the poly(U)/poly(A) concentration ratio of 2:1, a mixture of 2 poly(U)·poly(A) and poly(U)·poly(A) was observed in 1M NaClO₄, in contrast to the case of 1M NaCl. Thus, sodium perchlorate, a strong destabilizer of water structure, promotes formation of double-helical complexes both in the polynucleotide–monomer and the polynucleotide–polynucleotide systems. Beginning with a sufficiently high ionic strength (μ ? 0.9), a further increase in the salt molarity results in an increase of the poly(U)·adenosine melting temperature in both stabilizing and neutral salts and a decrease in the destabilizing salt. In Na₂SO₄ concentrations higher than 1.2M Ado·2 poly(U) precipitates at room temperature. Analysis of the binding isotherms and melting profiles of the complexes between poly(U) and adenosine according to Hill's model shows that the cooperativity of binding, due to adenosine stacking on poly(U), increases in the order NaClO₄ < NaCl < Na₂SO₄. The free energy of adenosine stacking on the template is similar to that of hydrogen bonding between adenosine and poly(U) and ranges from ?1 to ?2 kcal/mol. The values of ΔH_t [the effective enthalpy of adenosine binding to poly(U) next to an occupied site, obtained from the relationship between complex melting temperature and free monomer concentration at the midpoint of the transition] are ?14.2, ?18.3, and ?16.8 kcal/mol for 1M solutions of NaClO₄, NaCl, and Na₂SO₄, respectively. The results indicate that the effects of anions of the salts studied are related to water structure alterations rather than to their direct interaction with the complexes between poly(U) and adenosine.     

The binding of adenosine to polyuridylic acid in which uracil residues are chemically altered.

The binding of adenosine-¹⁴C to polyuridylic acid (poly(U)) and several modified poly(U)s has been studied by equilibrium dialysis. The poly(U) was modified by addition of appropriate reagents across the 5,6-double bond of the uracil ring to form the photohydrate, photodimer, dihydrouracil, the HOBr addition product and the HSO₃^? addition product. Modification of the uracil rings decreases the amount of adenosine which can be bound to the poly(U); the decrease in binding is a function of the fraction of uracil rings which have been changed. Using the expression S = S₀(1 ? αr)² to relate the fraction of uracil rings modified (r) to the number of binding “sites” remaining (S), it is found that α is about 1 for all the modifications except photodimer where it is about 2. These observations are taken to mean that the loss of binding capacity of the poly(U) resulting from modifications of the uracil ring is caused by loss of planarity of the uracil rings caused by the modifications, and consequent loss of double helix structure, but that for all modifications except photodimer there is no disruption of the poly(U) double helix on either side of the leison. There does appear to be local melting on either side of the photodimer lesion. The sigmoidal binding isotherms (A_b versus C_a) of modified and unmodified poly(U) can be approximated closely by the following equation: ((1)) (1) where A_b = bound A, C_a = free A, n = minimum number of adjacent A′s in complex, S = concentration of sites on poly(U), and K₁ = (K_m)^1/m for all m ≥ n. The stacking energy of adenosine (w) can be calculated accurately using the following equation, where dθ/d ln C_a is obtained from Eq. (1). ((2)) (2) For unmodified poly(U), w is ?2.0 kcal/mole and ΔG° (?;RT ln K₁) is ?3.2 kcal/mole. The difference (?1.2 kcal/mole) is attributed to hydrogen bonding. Heavily photohydrated poly(U) does not bind guanosine or guanosine-5′-phosphate.