Raman spectral studies of nucleic acids. XVI. Structures of polyribocytidylic acid in aqueous solution

Raman spectra of polyribocytidylic acid show the formation of an ordered single-stranded structure [poly(rC)] at neutral pH and an ordered double-stranded structure containing hemiprotonated bases [poly(rC)·poly(rC⁺)] in the range 5.5 > pH > 3.7. Below 40°C, poly(rC) contains stacked bases and a backbone geometry of the A-type, both of which are gradually eliminated by increasing the temperature to 90°C. Below 80°C, poly(rC)·poly(rC⁺) contains bases which are hydrogen bonded and stacked and a backbone geometry also of the A-type. In this structure the bases of each strand are shown to be structurally identical, i.e., hemiprotonated, and therefore distinct from both neutral and protonated cytosines. Infrared and Raman spectra indicate the existence of a center of symmetry with respect to the paired cytosine residues, which suggests that the additional proton per base pair is shared equally by the two hydrogen-bonded bases. Denaturation of poly(rC)·poly(rC⁺) occurs cooperatively (t_m ≈ 80°C) with elimination of base stacking, base pairing, and the A-helix geometry. Each of the separated strands of the denatured complex is shown to contain comparable amounts of both neutral and protonated cytosines, most likely in alternating sequence [poly(rC, rC⁺)]. In both poly(rC, rC⁺) and poly(rC), at 90°C, the backbones do not exhibit the phosphodiester Raman frequencies characteristic of other disordered polyribonucleotide chains. This is interpreted to mean that the single strands, though devoid of base stacking and A-type structure, contain uniformly ordered backbones of a specific type. Fully protonated poly(rC⁺), on the other hand, forms no ordered structure and may be characterized as a disordered (random chain) polynucleotide at all temperatures. Several Raman lines of poly(rC) are absent from the spectrum of poly(rC)·poly(rC⁺) and vice versa. These frequencies, assigned mainly to vibrations of the ribose groups, suggest that the furanose ring conformations are different in the single-stranded and double-stranded structures of polyribocytidylic acid. Several other Raman group frequencies have been identified and correlated with the polymer secondary structures.     

Raman studies of nucleic acids. XII. Conformations of oligonucleotides and deuterated polynucleotides

Laser Raman spectra of the trinucleoside diphoshate ApApA and dinucleoside phosphates ApU, UpA, GpC, CpG, and GpU are reported and discussed. Assignments of conformationally sensitive frequencies are-facilitated by comparison with spectra reported here of poly(rA), poly(rC), and poly(rU) in deuterium oxide solutions. The significant spectral differences between ApU and UpA, and between GpC and CpG, reveal that the sequence isomers have nonidentical conformations in aqueous solution. In UpA at low temperature the bases are stacked and the backbone conformation is similar to that found in ordered polynucleotide structures and RNA. In ApU no base stacking can be detected and the backbone conformation differs from that found in UpA, both in the orientation of phosphodiester linkages and in the internal conformation of ribose. At the conditions employed neither ApU nor UpA exhibits base pairing in aqueous solutions. In both GpC and CpG the bases are stacked and the phosphodiester conformations are similar to those encountered for UpA and RNA. However, major differences between spectra of GpC and CpG indicate that the geometries of stacking and ribosyl conformations are different. In GpC the Raman data favor the formation of hydrogen bonded dimers containing GC pairs. Protonation of C in GpC is sufficient to eliminate the ordered conformation detected by Raman spectroscopy. Despite the ordered backbone conformation evident in GpU, this dinucleoside apparently contains neither stacked nor hydrogen bonded bases at the conditions employed here. The Raman data also confirm the stacking interactions in ApApA, poly(rA), and poly(rC) but suggest that the backbone conformation in poly(rC) differs qualitatively from that found in most ordered polynucleotide structures and is thermally more stable. The present results demonstrate the sensitivity of the Raman technique to sequence-related structural differences in oligonucleotides and provide additional spectra–structure correlations for future conformational studies of RNA by laser Raman spectroscopy.     

Neighbor–neighbor interactions in single-strand polynucleotides: Optical rotatory dispersion studies of the ribonucleotide ApApCp

The neighbor–neighbor interactions in the small ribotrinucleotide ApApCp were investigated with the aid of optical rotatory dispersion measurements. This trinucleotide shows a Cotton effect between 220 and 325 mμ, in the region of its maximum ultraviolet absorption. The specific rotation of the trinucleotide is independent of concentration while the magnitude of the Cotton effect (levorotation) decreases markedly with increasing temperature. Such effects were not observed with the component nucleotides alone, in a simulated hydrolysis mixture, nor with the hydrolyzed trinucleotide. The Cotton effect is attributed to perturbation of the nucleotide base chromophores by neighbor–neighbor intramolecular interaction (stacking), without any hydrogen bonding being involved; this interaction decreases with increasing temperature because of increased internal rotational freedom about the single bonds of the backbone chain with an accompanying disruption of the neighbor–neighbor interaction between the bases. This explanation is supported by a statistical mechanical theory of neighbor-neighbor interactions in polynucleotides, involving the forces between the bases. Application of this technique to further studies of polynucleotides and polypeptides is discussed.     

5-Nitrouridine-monohydrate: crystal structure and conformation.

The crystal structure of 5-nitrouridine was determined by X-ray analysis. The pyrimidine ring is slightly non-planar, showing a shallow boat conformation. The nitro group has no influence on the C4 - O4 bond length as compared to uridine. The ribose shows the C3'-endo conformation and the base is in the anti orientation to the sugar with a torsion angle of 25.6 degrees. This conformation is stabilized by a hydrogen bond from the base to the ribosyl moiety (H6 ... 05'). Stacking interactions between neighboring bases are almost negligible in the crystal. A water molecule is involved in a bifurcated donating hydrogen bond to 04 and to 052 of the nitro group of the one base and an accepting bond from the H3 of the other base. Two more hydrogen bonds are formed between the water molecule and the ribose. The structural aspects of 5-nitrouridine are discussed with respect to the special stacking features found for 5-nitro-1-(beta-D-ribosyluronic acid)-uracil monohydrate in the crystal (1).     

Recognition of DNA substrates by T4 bacteriophage polynucleotide kinase

T4 phage polynucleotide kinase (PNK) displays 5′-hydroxyl kinase, 3′-phosphatase and 2′,3′-cyclic phosphodiesterase activities. The enzyme phosphorylates the 5′ hydroxyl termini of a wide variety of nucleic acid substrates, a behavior studied here through the determination of a series of crystal structures with single-stranded (ss)DNA oligonucleotide substrates of various lengths and sequences. In these structures, the 5′ ribose hydroxyl is buried in the kinase active site in proper alignment for phosphoryl transfer. Depending on the ssDNA length, the first two or three nucleotide bases are well ordered. Numerous contacts are made both to the phosphoribosyl backbone and to the ordered bases. The position, side chain contacts and internucleotide stacking interactions of the ordered bases are strikingly different for a 5′-GT DNA end than for a 5′-TG end. The base preferences displayed at those positions by PNK are attributable to differences in the enzyme binding interactions and in the DNA conformation for each unique substrate molecule.     

Anti-cooperative interactions in single-strand oligomers of deoxyriboadenylic acid

Optical rotatory dispersion measurements were made on the deoxyribo nucleotides d(pA)₂, d(pA)₄, d(pA)₆ and poly(deoxyriboadenylic acid) at neutral pH over the temperature range 5–80°C. and were compared to similar data for the analogous oligoriboadenylic acids. The data were interpreted in terms of a temperature-dependent stacking of the bases in the single-strand deoxyribo oligomers. The thermal transition curves show an inverted chain-length dependence compared to the ribo oligomer curves. These results are explained by a theory of anti-cooperative interaction, where the nucleation parameter σ is >1. The theory, based on a one-dimensional Ising model involving both attractive nearest-neighbor and repulsive next-nearest-neighbor interactions, predicts the inverse chain length dependence and agrees rather well with the experimental data. At and above the transition temperature, the deoxyribo polymer is seen to consist of isolated stacked base pairs separated by at least one unit of random coil, there being only a very small probability for the existence of sequences of stacked residues longer than one. The partition function is seen to undergo an irregular behavior as a function of chain length because of the anti-cooperative phenomenon. It is necessary to use an enthalpy of stacking of ?5.0 kcal./mole in order to fit the experimental data with the theory. This value, 1.5 kcal./mole more positive than the ΔH found for the ribo oligomers, is reasonable, since the 2′ hydroxyl group would be expected to stabilize the stacking interaction in the ribo oligomers. Various kinds of distribution functions are calculated and plotted graphically for this theoretical model. A physical rationale is presented for the use of a repulsive next-nearest-neighbor term in this theory for the deoxyribo oligomers.     

Modification of ribonucleic acid by chemical carcinogens. VI. Effect of N-2-acetylaminofluorene modification of guanosine on the codon function of adjacent nucleosides in oligonucleotides

Oligonucleotides containing a guanosine residue on the 5′ or the 3′ side of tri- and tetranucleotides were prepared. The guanosine residue was modified with the chemical carcinogen N-2-acetylaminofluorene and the control and modified oligonucleotides were tested for their ability to stimulate ¹⁴C-labeled amino-acyl-tRNA binding to ribosomes. The effects of the modification are twofold. The first is that if the guanosine residue to which the drug is eovalently bound is part of a codon the oligonucleotide is completely inactive in the ribosomal binding assay. The second is that if an adenosine residue is adjacent to either the 5′ or 3′ side of the modified guanosine, as in (Ap)₃G or G(pA)₃, there is partial inhibition of ¹⁴C-labeled lysyl-tRNA binding to ribosomes. This inhibitory effect extends only to the function of the immediately adjacent adenosine since the chemical modification of guanosine residues in (Ap)₄G or G(pA)₄ did not impair their ability to code for lysine. In contrast to these findings if there is a uridine residue adjacent to the modified guanosine, as in (Up)₃G or G(pU)₃ there is no effect on ¹⁴C-labeled phenylalanyl-tRNA binding to ribosomes. Proton magnetic resonance spectra of UpG, GpU and the corresponding dinners in which the guanosine residue was modified with the drug failed to indicate a stacking interaction between the fluorene moiety and the adjacent uridine residue. This is in contrast to previous studies demonstrating a strong stacking interaction between fluorene and adjacent adenosine residues. Taken together these results indicate that acetylaminofluorene modification of guanosine next to an adenosine residue in oligonucleotide inhibits its ribosomal binding capacity. The stacking interaction with adjacent adenosine, and not with adjacent uridine residues, in oligonucleotides probably accounts for the effects observed in the ribosomal binding assay. These data are consistent with our previously described “base displacement” model.     

Investigation of the base-pairing structure of the anticodon hairpin from E. coli initiator tRNA by high-resolution nmr

The high-resolution nmr spectrum of the anticodon hairpin from E. coli tRNA^fMet has been obtained at a number of different temperatures. The positions of the resonances from interior Watson-Crick base pairs are well accounted for (within 0.1 ppm) by a semi-empirical ring current shift theory, but the terminal base pairs are susceptible to the exact orientation of adjacent bases in single-stranded regions. From a careful examination of the exact way in which resonances disappear at elevated temperatures, we conclude that melting in the nmr experiments occurs when the lifetime of a base pair is reduced to several milliseconds. On the basis of these experiments we are able to assign an nmr T_m to each individual base pair and these should be useful in interpreting the melting behavior of the intact molecule. An “extra” resonance is observed at ～11.3 ppm and, on the basis of its position and temperature sensitivity, it is tentatively assigned to the ring nitrogen proton of a “protected” U residue in the anticodon loop. A strong preference for stacking of a nonbase-paired A residue on an adjacent GC base pair is observed even at temperatures in excess of 52°C.     

Conformational features of benzo‐homologated yDNA duplexes by molecular dynamics simulation

yDNA is a base‐modified nucleic acid duplex containing size‐expanded nucleobases. Base‐modified nucleic acids could expand the genetic alphabet and thereby enhance the functional potential of DNA. Unrestrained 100 ns MD simulations were performed in explicit solvent on the yDNA NMR sequence [5′(yA T yA yA T yA T T yA T)₂] and two modeled yDNA duplexes, [5′(yC yC G yC yC G G yC G G)₂] and [(yT5′ G yT A yC yG C yA yG T3′)?(yA5′ C T C yG C G yT A yC A3′)]. The force field parameters for the yDNA bases were derived in consistent with the well‐established AMBER force field. Our results show that DNA backbone can withstand the stretched size of the bases retaining the Watson‐Crick base pairing in the duplexes. The duplexes retained their double helical structure throughout the simulations accommodating the strain due to expanded bases in the backbone torsion angles, sugar pucker and helical parameters. The effect of the benzo‐expansion is clearly reflected in the extended C1′‐C1′ distances and enlarged groove widths. The size expanded base modification leads to reduction in base pair twist resulting in larger overlapping area between the stacked bases, enhancing inter and intra strand stacking interactions in yDNA in comparison with BDNA. This geometry could favour enhanced interactions with the groove binders and DNA binding proteins., 2016. © 2015 Wiley Periodicals, Inc. Biopolymers 105: 55–64, 2016     

An analysis of the results for the binding of formaldehyde to polyuridylic acid

Spectrophotometric measurements were made on the extent of binding of formaldehyde to polyuridylic acid under conditions of varying temperature and formaldehyde concentration. The data is interpreted in terms of a temperature-dependent stacking of the bases in poly U at 20°, but not at 40°C. A theory of cooperative stacking is developed which considers the base residues to be either non-bonded, non-bonded and methylolated, or stacked. The results indicate essentially non-cooperative base stacking under these conditions with an equilibrium constant for base stacking of 0.92 at 20°C.     

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.     

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.     

Conformational dependence of the Raman scattering intensities from polynucleotides. 3. Order-disorder changes in helical structures

Raman spectra are presented on ordered and presumably helical structures of DNA and RNA as well as the poly A·poly U helical complex, polydAT, and the helical aggregates of 5′-GMP and 3′-GMP. The changes in the frequency and the intensity of the Raman bands as these structures undergo order-disorder transitions have been measured. In general the changes we have found can be placed into three categories: (1) A reduction in the intensities of certain ring vibrations of the polynucleotide bases is observed when stacking or ordering occurs (Raman hypochromism). Since the ring vibrational frequencies are different for each type of base, we have been able to obtain some estimate of average amount of order of each type of base in partially ordered helical systems. (2) A very large increase in the intensity of a sharp, strongly polarized band at about 815 cm^?1 is observed when polyriboA and polyriboU are formed into a helical complex. Although this band is not present in the separated chains at high temperature, a broad diffuse band at about 800 cm^?1 is present. The 815 cm^?1 band undoubtedly arises from the vibrations of the phosphate-sugar portions of the molecule and provides a sensitive handle to the back-bone conformation of the polymer. This band also appears upon ordering of RNA, formation of the helical aggregate of 5′-riboGMP, and to some extent in the selfstacking of the polyribonucleotides polyA, polyU in the presence of Mg⁺⁺, PolyC, and polyG. No such intense, polarized band is found, however, in ordered DNA, polydAT, or the 3′-riboGMP aggregate, although there is a conformationally independent band at about 795 cm^?1 in DNA and polydAT. (3) Numerous frequency changes occur during Conformational changes. In particular the 1600–1700 cm^?1 region in D₂O shows significant conformationally dependent changes in the C?O stretching region analogous to the changes in this region which have been observed in these substances in the infrared. Thus, Raman scattering appears to provide a technique for simultaneously observing the effects of base stacking, backbone conformation and carbonyl hydrogen bonding in nucleic acids in moderately dilute (10–25 mg/ml) aqueous solutions.     

Raman spectroscopy of interferon-induced 2',5'-linked oligoadenylates

Raman spectra of model compounds and of 2',5'-oligoadenylates in D2O were utilized to assign the Raman bands of 2',5'-oligoadenylates. The Raman spectra of A2'pA2'pA, pA2'pA2'pA, and pppA2'pA2'pA contained features that were similar to those of adenosine, adenosine 5'-monophosphate (AMP), and adenosine 5'-triphosphate, respectively. When AMP and pA2'pA2'pA were titrated from pH 2 to 9, the normalized Raman intensity of their ionized (980 cm-1) and protonated (1080 cm-1) phosphate bands revealed similar pKa's for the 5'-monophosphates. The Raman spectrum of pA2'pA2'pA was altered slightly by elevations in temperature, but not in a manner supporting the postulate that 2-5A possesses intermolecular base stacking. Major differences in the Raman spectrum of 2',5'- and 3',5'-oligoadenylates were observed in the 600-1200-cm-1 portion of the spectrum that arises predominately from ribose and phosphate vibrational modes. Phosphodiester backbone modes in A3'pA3'pA and pA3'pA3'pA produced a broad band at 802 cm-1 with a shoulder at 820 cm-1, whereas all 2',5'-oligoadenylates contained a major phosphodiester band at 823 cm-1 with a shoulder at 802 cm-1. The backbone mode of pppA2'pA2'pA contained the sharpest band at 823 cm-1, suggesting that the phosphodiester backbone may be more restrained in the biologically active, 5'-triphosphorylated molecule. The Raman band assignments for 2',5'-oligoadenylates provide a foundation for using Raman spectroscopy to explore the mechanism of binding of 2',5'-oligoadenylates to proteins.     

Theoretical studies on protein-nucleic acid interactions. III. Stacking of aromatic amino acids with bases and base pairs of nucleic acids

Stacking of aromatic amino acids tryptophan (Trp), tyrosine (Tyr), phenylalanine (Phe), and histidine (His) with bases and base pairs of nucleic acids has been studied. Stacking energies of the amino acid–base (or base pair) complexes have been calculated by second-order perturbation theory. Our results show that, in general, the predominant contribution to the total stacking energy comes from the dispersion terms. In these cases, repulsion energy is greater than the sum of electrostatic and polarization energies. In contrast to this, interaction of histidine with the bases and base pairs is largely Coulombic in nature. The complexes of guanine with aromatic amino acids are more stable than the corresponding complexes of adenine. Among pyrimidines, cytosine forms the most stable complexes with the aromatic amino acids. The G · C base pair has the highest affinity with aromatic amino acids among various sets of base pairs. Optimized geometries of the stacked complexes show that the aromatic moieties overlap only partially. The heteroatom of one residue generally overlaps with the other aromatic moiety. There is a considerable degree of configurational freedom in the stacked geometries. The role of stacking in specific recognition of base sequences by proteins is discussed.     

The spatial configuration of ordered polynucleotide chains. I. Helix formation and base stacking.

A single virtual bond scheme set forth previously for the treatment of average properties of randomly coiling polynucleotides is here applied to the calculation of helical parameters which characterize a regularly repeating polynucleotide molecule. Only a fraction of the enormous number of conformationally feasible helixes fulfill the geometric criteria of vertical base stacking usually associated with ordered polynucleotide chains. Detailed examination of the nature and mode of base stacking feasible in a single helical backbone structure indicates that the handedness of a base stacking arrangement does not correlate either quantitatively or qualitatively with the handedness of the polymer backbone. A number of polynucleotide chains which exhibit lefthanded base stacking patterns in nmr and CD studies may, in fact, be righthanded helixes.     

Loop Stereochemistry and Dynamics in Transfer RNA

Abstract

The stereochemistry and the dynamics of two loops of yeast tRNA-asp, the thymine loop and the anticodon loop, are compared in the hope of a better understanding of the relationships between loop sequence and loop topology. Both loops are seven residues long and both present sharp turns after the second residue, U33 and ψ55, stabilized by hydrogen bonds between N3-H of the pyrimidine and the phosphates of C36 and A58 and stacking interactions of the pyrimidine ring with the phosphates of U35 and A57, respectively. In the thymine loop, the two purines following C56, A57 and A58, open up to leave space for the intercalation of the first invariant guanine residue of the D-loop, while the two pyrimidine bases, which follow A58, turn away from the stacking pattern of the thymine arm and stack instead with the last base pair of the dihydrouridine arm A15-U48. In the anticodon loop, however, the bases G34 to C38 form an helical stack in continuity with the anticodon stem on the 3′-end. At the same time C36 forms Watson-Crick hydrogen bonds with G34 of a twofold symmetrically related molecule. The anticodon-anticodon base pairing interactions between symmetrically-related molecules are stabilized by stacking with the modified base G37 on both sides of the triplet. Some comparisons are made with the structure of yeast tRNA-phe and some implications about the structure of mitochondrial tRNAs are discussed.     

Syn–anti equilibrium of purine bases in dinucleoside monophosphates as studied by proton longitudinal relaxation

The preferential orientations of the purine bases in dinucleoside monophosphates such as ApA, ApG, and GpA in 10^?2M neutral aqueous solutions have been investigated by proton relaxation at 250 MHz. These orientations are deduced from computer simulations of the magnetization recovery curves following a 180° nonselective pulse. The distances between the H(8) proton of a base and the ribose ring protons which are used in these calculations are obtained by minimization as a function of the glycosyl torsion angle ? of the standard deviation between the isotropic reorientation correlation times τ_R derived from the relaxation rates of these protons. The average H(1′) – H(8) distance obtained by this procedure may be readily verified from the reduction of the H(1′) relaxation rate when H(8) is substituted by a deuteron. The limits of validity of the assumption of a single correlation time τ_R governing the proton relaxation have been estimated, taking into account several possible internal motions, e.g., the rotation of the base, of the methylene exocyclic group and the N ? S interconversion of the ribose ring. For 10^?10 < τ_R < 2 × 10^?10 sec, it appears that the influence of these motions on the proton relaxation becomes perceptible when the jump rates among equilibrium positions exceed ca. 10⁹ sec^?1. The whole of the experimental results show that for the ribose ring N conformer, the orientation of the bases is found in the ranges 60° < ? < 80° (syn) and 180° < ? < 210° (anti). For ribose S conformer, it is observed that this orientation is mainly syn with 5° < ? < 90°. The average H(1′) – H(8) distance provides semiquantitative information on the overall syn or anti orientations of the base in each nucleoside moiety. At 298 K the population of the anti conformer is found to increase in the order A- pG < Ap -G ～ Gp -A < Ap -A < A-pA < G-pA . A more detailed analysis of relaxation data shows that the maximum possible fraction of the stacked form of dinucleotides, due to the occurrence of N-anti conformers in both nucleoside moieties, is in the order ApG < GpA < ApA, in agreement with previous works, with however smaller values. Lastly the deuteron linewidth in position 8 of the bases indicates a syn–anti transition rate of the order of 10⁹ sec^?1 at room temperature, without noticeable effects therefore on the proton relaxation.     

Indole ring binds to 7-methylguanine base by pi-pi stacking interaction. Crystal structure of 7-methylguanosine 5'-monophosphate-tryptamine complex

Strong pi-pi stacking interaction between the indole ring and 7-methylguanine base was shown by X-ray crystal analysis of the 7-methylguanosine 5'-monophosphate-tryptamine complex. This interaction appears to be strengthened by the attachment of ribose and phosphate groups to the base.     

A proton magnetic resonance study of the interaction of adenylyl (3' is greater than 5') adenosine with polyuridylic acid

The interaction of adenylyl (3′ → 5′) adenosine (ApA) with polyuridylic acid in D₂O solution at neutral pD has been studied by high resolution proton magnetic, resonance spectroscopy. At temperatures above ～32°C, no evidence was obtained for the interaction of ApA with poly U. Below this temperature, a rigid triple-stranded complex involving a stoichiometry of 1 adenine to 2 uracil bases is formed, presumably via specific adenine–uracil base-pairing and cooperative base stacking of the adenine bases in a manner similar to that previously reported for the adenosine–poly U complex.