Conformational features of 2′-O-methyl-adenosylyl-adenosine

In order to obtain information about the conformational features of a 2′-O-methylated polyribonucleotide at the nearest neighbor level, a detailed nuclear magnetic resonance study of AmpA was undertaken. AmpA was isolated from alkali hydrolysates of yeast RNA, and proton spectra were recorded at 100 MHz in the Fourier transform mode in D₂O solutions, 0.01 M, pH 5.4 and 1.5 at 25°C. ³¹P spectra were recorded at 40.48 MHz. Complete, accurate sets of nmr parameters derived for each nucleotidyl unit by simulation iteration methods. The nmr data were translated into conformational parameters for all the bonds using procedures developed in earlier studies from these laboratories. It is shown that AmpA exists in aqueous solution with a flexible molecular framework, which shows preferences for certain orientations. The ribose rings exist as a ²E ? ³E equilibrium with the —pA ribose showing a bias for the ³E pucker. The C(4′)—C(5′) bonds of both nucleotidyl units show significant preference (75–80%) to exist in gg conformation. The dominant conformer (80%) about C(5′)—O(5′) of the 5′-nucleotidyl unit is g′g′. Even though an unambiguous determination of the orientation of the 3′-phosphate group cannot be made, tentative evidence shows that it preferentially occupies g⁺ domains [O(3′)—P trans to C(3′)—C(2′)] in which the H(3′) —C(3′)—O(3′)—P(3′) dihedral angle is about 31°. There is reasonable evidence that the 2′-O-methyl preferentially occupies the domain in which the O(2′)—CH₃ bond is trans to C(2′)—C(1′). Lowering of pH to 1.5, which results in protonation of both the adenine moieties, causes destacking of AmpA. Such destacking is accompanied by small, but real, perturbations in the conformations about most of the bonds in the backbone. A detailed comparison of the solution conformations of ApA and AmpA clearly shows that 2′-O-methylation strongly influences the conformational preference about the C(3′)—O(3′) bond of the 3′-nucleotidyl unit, in addition to inducing small changes in the overall ribophosphate backbone conformational equilibria. The effect of 2′-O-methylation is such that the C(3′)—O(3′) is forced to occupy preferentially the g⁺ domain rather than the normally preferred g^? domain [O(3′)—P trans to C(3′)—C(4′)] in ApA. The data on ApA and AmpA further reveal that the extent of stacking interaction is less in AmpA compared to ApA. It is suggested that stacked species of AmpA exist as right-handed stacks where the magnitude of ω and ω′ about O(5′)—P and P—O(3′) is about 290°. The reason for the lesser degree of stacking in AmpA compared to ApA is intramolecular interaction between 2′-O-methyl and the flexible O(3′)—P—O(5′) bridge, the interaction causing some perturbation in the magnitudes of ω/ω′, causing destacking. The destacking will lead to an increase in _χCN by a few degrees, causing an increase in ²E populations; the latter in turn will shift the 3′ phosphate group from g^? to g⁺ domains. In short, a coupled series of conformational events is envisioned at the onset of destacking, made feasible by the interaction between the 2′-O-methyl group and the swivel O(3′)—P—O(5′) bridge.     

Influence of ribose 2′-O-methylation on GpC conformation by classical potential energy calculations

Potential energy calculations were employed to examine the effect of ribose 2′-O-methylation on the conformation of GpC. Minimum energy conformations and allowed conformational regions were calculated for 2′MeGpC and Gp2′MeC. The two lowest energy conformations of 2′MeGpC and Gp2′MeC are similar to those of GpC itself. The helical RNA conformation (sugar pucker-C(3′)-endo, ω′ and ω,g^?g^?, bases-anti) is the global minimum, and a helix-reversing conformation with ω′, ω in the vicinity of 20°, 80° is next in energy. However, subtle differences between the three molecules are noted. When the substitution is on the 5′ ribose (Gp2′MeC), the energy of the helical conformation is less than that of GpC, due to favorable interactions of the added methyl group. When the substitution is at the 3′ ribose (2′MeGpC) these stabilizing interactions are outweighed by steric restrictions, and the helical conformation is of higher energy than for GpC. Furthermore, the statistical weight of the 2′MeGpC g^? g^? helical region is substantially less than the corresponding weight for Gp2′MeC. In addition, 2′MeGpC′s methoxy group is conformationally restricted to a narrow range centered at 76°. This group has a broadly allowed region between 50 and 175° in Gp2′MeC. These differences occur because the appended methyl group in 2′MeGpC is located in the interior of the helix cylinder, as it would be in polynucleotide, while it hangs unimpeded in Gp2′MeC. These findings suggest that 2′-O-methylation has both stabilizing and destabilizing influences on the helical conformation of RNA. For 2′MeGpC the destabilizing steric hindrance imposed by the nature of the guanine base dominates.     

Examination by the molecular orbital method of the intrinsic conformation preferences of nucleic acid sequence]

This paper reports a systematic PCILO study of the conformation of the nucleic acid backbone. The authors principally studied the ω′ and ω phosphodiester torsion angles of the disugar triphosphate model as a simultaneous function of (1) the sugar nature, ribose or deoxyribose, (2) the different combinations of the sugar ring puckers C(2′)-endo-C(2′)-endo, C(3′)-endo-C(3′)-endo, C(3′)-endo-C(2′)-endo, and C(2′)-endo-C(3′)-endo, and (3) the different conformations around the ψ(C4′–C5′) exocyclic bond. The dependence of the (ω′,ω) conformational energy maps upon these different factors, is discussed. The results are in very good agreement with the observed structures of ribonucleic (RNA10, RNA11, A′-RNA12, tRNA^Phe) and deoxyribonucleic acids (D-DNA, C-DNA 9.3, B-DNA 10, A-DNA 11). Thus the validity of this model, the disugar triphosphate unit, is ensured. The main conclusions that can be drawn from this systematic study are the following:

• 1 The torsion around P-05′ (angle ω) is, as a general rule, more flexible than the torsion around P-03′ (angle ω′).
• 2 There is no notable difference between the ribose–triphosphate units and the deoxyribose–triphosphate units for the C(3′)-endo–C(3′)-endo and C(3′)-endo–C(2′)-endo sugar puckers.
• 3 The deoxyribose–triphosphate units with C(2′)-endo–C(2′)-endo and C(2′)-endo–C(3′)-endo sugar puckers show much more ω′ flexibility than the ribose–triphosphate units with the same sugar puckers and cis position for the 2′hydroxyl group.
• 4 The preferred values of ω′ are independent of the sugar nature (ribose or deoxyribose) and of ψ values; they are correlated with the sugar pucker of the first sugar-phosphate unit:
  • C(3′)-endo-C(3′)-endo and C(3′)-endo-C(2′)-endo puckers ? ω′ ? 240° (g^? region)
  • C(2′)-endo-C(2′)-endo and C(2′)-endo-C(3′)-endo puckers ? ω′ 180° (t region)
• 5 The preferred values of ω are independent of the nature and the puckering of the sugars; they are correlated with the rotational state of the torsion angle ψ(C4′–C5′): ψ ? 60° (gg) ? ω ? 300° (g^?), ψ ? 180° (gt) or 300° (tg) ? ω ? 60° (g⁺)

     

Backbone conformations in deoxyribonucleic acids. Conformational role of the 2′-hydroxyl group on the internucleotide phosphodiester conformations

The conformations accessible to the internucleotide phosphodiester group in deoxydinucleoside monophosphates, deoxydinucleoside triphosphates, and deoxypolynucleotides have been explored in detail by potential energy calculations. The two most predominant conformations for the nucleotide moiety (³E and ²E) and their possible combinations (³E^?3E, ³E^?2E, ²E^?2E, ²E^?3E) have been employed, similar to our earlier studies on polyribonucleotides. The internucleotide P-O bond torsions are very sensitive to the sugar pucker (³E and ²E) and sugar type (ribose and 2′-deoxyribose) on the 3′-residue of dinucleoside phosphates. The preferred phosphodiester conformations found for the deoxydinucleoside monophosphates and triphosphates, in general, follow the same pattern as those obtained for ribose sugars when the sugar on the 3′-side of the molecule has the ³E sugar-ring conformation. The internucleotide P-O bonds show a greater degree of conformational freedom when the 3′-sugar has the ²E pucker. The double gauche g^?g^? conformation for the phosphodiester, which leads to the overlap of the adjacent bases, is shown to be one of the energetically most favored conformations for all the sequence of sugar puckers. It is found that the ²E^?2E sequence of sugar puckers shows a greater energetic preference for the stacked helical conformation (g^?g^?) than the (³E^?3E) and the mixed sugar-pucker combinations. This effect becomes more pronounced in going from a dinucleoside monophosphate to a dinucleoside triphosphate suggesting that the 2′-deoxy sugars favor the ²E sugar pucker in di-, oligo-, and polydeoxyribonucleotide structures. In addition to g^?g^?, the conformations g⁺g^?, tg^?, g^?t, tg⁺, and g⁺t are also found to be possible for the phosphodiester in a polydeoxyribonucleotide and their populations depend to some extent on the sugar-pucker sequence. It is shown that the short-range intramolecular interactions involving the sugar and the phosphate groups dictate to a large extent the backbone conformations of nucleic acids and polynucleotides.     

A Raman and calorimetric investigation of 3′, 5′ GpG

The Raman spectra of guanylyl (3′-5′) guanosine (GpG) in solution in H₂O and D₂O at pH 3–7 have been recorded at various temperatures between 0 and 80°C. The results are consistent with the existence in the lower temperature range of stable aggregates formed by the stacking of GpG tetramers. The aggregates melt cooperatively near 60°C, which results in important changes in the spectra. Among these, a large increase in intensity of some of the bands assigned to the guanine residues shows that unstacking of the bases occurs at the melting. Also apparent in the spectra are changes in the intensity and frequency of band attributable to molecular groups involved in intermolecular hydrogen bonding between adjacent molecules in the complex. The melting temperature of GpG decreases by approximately 15°C upon lowering the concentration from 5 × 10^?2 to 5 × 10^?4M, as shown by Raman, calorimetric, CD, and uv measurements. The experimentally determined ΔH and ΔS for the melting transition are 9 Kcal/mol and 28 e.u./mol, respectively. The aggregation of GpG in 1.5 × 10^?3M solutions was found to be very slow. The half-time of the process, which roughly follows first-order kinetics, is approximately 3 min at 10°C and 21 min at 35°C. The negative energy of activation associated with this reaction (?143 Kcal) indicated that the process involves intermediates whose concentrations decrease the temperatures raised, thus slowing down the overall process. The rate of disaggregation of GpG upon dilution to very low concentration is also extremely slow, indicating that the GpG aggregates, once formed, are very stable.     

Effect of O(2′)-methylation on the stability of polynucleotide helices

The effect of ribose(O2′)-methylation on the stability of (O2′)-methylated polyribonucleotide helices has been studied by conformational energy calculations. The preferred orientation of the methyl group is found to further stabilize the helical phosphodiester conformation (g^?,g^?) due to the enhanced short-range interactions arising between the methyl groups and the adjacent ribose moieties. The experimentally observed increase in melting temperature of (O2′)-alkylated polyribonucleotides is thus attributable to the enhanced stability of the helical backbone conformation.     

DFT study of geometrical and vibrational features of a 3′,5′-deoxydisugar-monophosphate (dDSMP) DNA model in the presence of counterions and solvent

The B3LYP/6–31++G* theoretical level was used to study the influence of various hexahydrated monovalent (Li⁺, Na⁺, K⁺) and divalent (Mg²⁺) metal counterions in interaction with the charged PO₂^? group, on the geometrical and vibrational characteristics of the DNA fragments of 3′,5′-dDSMP, represented by four conformers (g⁺g⁺, g⁺t, g^?g^? and g^?t). All complexes were optimized through two solvation models [the explicit model (6H₂O) and the hybrid model (6H₂O/Continuum)]. The results obtained established that, in the hybrid model, counterions (Li⁺, Na⁺, K⁺, Mg²⁺) always remain in the bisector plane of the O1–P–O2 angle. When these counterions are explicitly hydrated, the smallest counterions (Li⁺, Na⁺) deviate from the bisector plane, while the largest counterions (K⁺ and Mg²⁺) always remain in the same plane. On the other hand, the present calculations reveal that the g⁺g⁺ conformer is the most stable in the presence of monovalent counterions, while conformers g⁺t and g^?t are the most stable in the presence of the divalent counterion Mg²⁺. Finally, the hybrid solvation model seems to be in better agreement with the available crystallographic and spectroscopic (Raman) experiments than the explicit model. Indeed, the six conformational torsions of the C4′-C3′-O3′-PO^?₂-O5′-C5′-C4′ segment of all complexes of the g^?g^? conformer in 6H₂O/Continuum remain similar to the available experimental data of A- and B-DNA forms. The calculated wavenumbers of the g⁺g⁺ conformer in the presence of the monovalent counterion and of g^?t conformer in presence of the divalent counterion in the hybrid model are in good agreement with the Raman experimental data of A- and B-DNA forms. In addition, the maximum deviation between the calculated wavenumbers in the 6H₂O/Continuum for the g⁺g⁺ conformer and experimental value measured in an aqueous solution of the DMP-Na⁺ complex, is <1.07% for the PO₂^? (asymmetric and symmetric) stretching modes and <2.03% for the O5′-C5′ and O3′-C3′ stretching modes.

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Graphical abstract dDSMP-(OO)^? Mg²⁺/6W/Continuum

     

Mn‐Rich P′2‐Na0.67[Ni0.1Fe0.1Mn0.8]O2 as High‐Energy‐Density and Long‐Life Cathode Material for Sodium‐Ion Batteries

Herein, P′2‐type Na_0.67[Ni_0.1Fe_0.1Mn_0.8]O₂ is introduced as a promising new cathode material for sodium‐ion batteries (SIBs) that exhibits remarkable structural stability during repetitive Na⁺ de/intercalation. The O? Ni? O? Mn? O? Fe? O bond in the octahedra of transition‐metal layers is used to suppress the elongation of the Mn? O bond and to improve the electrochemical activity, leading to the highly reversible Na storage mechanism. A high discharge capacity of ≈220 mAh g^?1 (≈605 Wh kg^?1) is delivered at 0.05 C (13 mAg^?1) with a high reversible capacity of ≈140 mAh g^?1 at 3 C and excellent capacity retention of 80% over 200 cycles. This performance is associated with the reversible P′2–OP4 phase transition and small volume change upon charge and discharge (≈3%). The nature of the sodium storage mechanism in a full cell paired with a hard carbon anode reveals an unexpectedly high energy density of ≈542 Wh kg^?1 at 0.2 C and good capacity retention of ≈81% for 500 cycles at 1 C (260 mAg^?1).     

Self-assembly of dideoxyguanosine (3′,3′) and (5′,5′)-monophosphates

The title compounds show a pronounced cation-directed ability to self-assemble in water and to gives columnar structures similar to four-stranded helices; for compound (5′→5′)-d(GpG), this leads to the formation of cholesteric and hexagonal liquid crystalline phases. Both phases are columnar and the cholesteric phase is left-handed. This behaviour is a further confirmation of the tendency of guanine derivatives to self-assemble to give stacked columnar structures whenever not impossible for structural reasons. The CD spectra of the aggregates in isotropic solutions are dominated by a negative exciton couplet centred around 250 nm associated to a left-handed columnar chirality. The shapes of the profiles, in the 220–300-nm region, for (5′→5′)-d(GpG) (in water or in saline solutions) and for (3′→3′)-d(GpG) (in KCl solution) are quasi-mirror images of those of poly(G) and (3′→5′)-d(GpG). The appearance of relatively intense CD signals around 280–300 nm in solution of (3′→3′)-d(GpG) in the presence of NaCl resembles that of (3′→5′)-d(GpG) in the presence of Rb⁺ or Na⁺. In the compounds investigated in this work, which present two equivalent ends, one observes the two CD features that have been associated, in the current literature, with the signature of four-stranded parallel and antiparallel structures: hence the origin of these CD bands cannot be found in the polarity of the strands. Self-assembly is favoured by the addition of extra salt and the stabilising effect of K⁺ is greater than that of Na⁺, in the case of (3′→3′)-d(GpG), an assembled species could be detected by CD only in the presence of extra salt. Chirality 10:734–741, 1998. © 1998 Wiley-Liss, Inc.     

Conformational study of ribonucleotides, 2′-deoxyribonucleotides,and arabinonucleotides by carbon-13 nuclear magnetic resonance

The geminal and vicinal ¹³C-³¹P coupling constants have been monitored, as a function of pH, for a series of uracil and cytosine 3′- and 5′-nucleotides with a ribose, arabinose, or 2′-deoxyribose sugar. Data were also obtained for two 3′,5′-diphosphates in the ribose and arabinose series. The geminal J(C5′-P5′) and J(C3′-P3′) couplings show only a small dependence on the ionization state of the phosphate, decreasing by < 0.5 Hz in the pH 5–7 range. For the ribose and arabinose 3′-nucleotides, the vicinal J(C4′-P3′) increase (up to 1.5 Hz) on secondary phosphate ionization in the pH 5–7 range, whereas their J(C2′-P3′) couplings decrease (up to 1.5 Hz) over the same pH range. In contrast for the 2′-deoxyribose molecules, both couplings decrease (～0.5 Hz) on phosphate ionization. The titration curves provide information about the influence of the sugar on the conformation about the C3′? O3′ bond. Some conformational trends could be rationalized by consideration of the sugar-puckerdependent contact interactions between the 3′-phosphate and the substituents on the furanose ring.     

Mutational tests of the NMR-docked structure of the staphylococcal nuclease–metal–3′,5′-pdTp complex

In the X-ray structure of the staphylococcal nuclease–Ca²⁺ ?3′,5′-pdTp complex, the conformation of the inhibitor 3′,5′-pdTp is distroteed Lys-70* and Lys-71* from an adjacent molecule of staphylococcal nuclease (Loll, P.J., Lattman, E.E. Proteins 5 : 183-201, 1989). In order to correct this crystal packing problem, the solution conformation of enzyme-bound 3′,5′-pdTp in the staphylococcal nuclease–metal–pdTp Complex determined by NMR methods was docked into the X-ray structure of the enzyme [Weber, D. J., Serpersu, E. H., Gittis, A. G., Lattman, E. E., Mildvan, A. S. (preceding paper)]. In the NMR-docked structure, the 5′-phophate of 3′,5′-pdTp overlaps with that in the X-ray Structure. However the 3′-phosphate accepts a hydrogen bond from Lys-49 (2.89Å) rather than from Lys-84 (8.63 Å), and N3 of thymine donates a hydrogen bond to the OH of Tyr-115 (3.16 Å) which does not occur in the X-ray structure (5.28 Å). These interactions have been tested by binding studies of 3′,5′-pdTp, Ca²⁺, and Mn²⁺ to the K49A, K84A, and Y115A mutants of staphylococcal nuclease using water proton relaxation rate and EPR methods. Each mutant was fully active and structurally intact, as found by CD and two-dimensional NMR spectroscopy, but bound Ca²⁺ 9.1- to 9.9-fold more weakly than the wild-type enzyme. While thye K84A mutation did not significantly weaken 3′,5′-pdTp binding to the enzyme (1.5 ± 0.7 fold), the K49A mutation weakened 3′,5′-pdTp binding to the enzyme by the factor of 4.4 ± 1.8-fold. Similarly, the Y115A mutation weakened 3′,5′-pdTp binding to the enzyme 3.6 ± 1.6-fold. Comparable weakening effects of these mutations were found on the binding of Ca²⁺-3′,5′-pdTp. These results are more readily explained by the NMR-docked structure of staphylococcal nuclease-metal-3′,5′-pdTp than by the X-ray structure. © 1993 Wiley-Liss, Inc.     

Configurational effects on conformational properties of cyclic nucleotides. I. Theoretical calculations of conformer preferences in α-nucleoside 3′,5′ cyclic monophosphates

A comparative study has been made of the configurational effects on the conformational properties of α- and β-anomers of purine and pyrimidine nucleoside 3′,5′,-cyclic monophosphates and their 2′-arabino epimers. Correlation between orientation of the base and the 2′-hydroxyl group have been studied theoretically using the PCILO (Perturbative Configuration Interaction using Localized Orbitals) method. The effect of change in ribose puckering on the base-hydroxyl interaction has also been studied. The result show that steric repulsions and stabilizing effects of intramolecular hydrogen bonding between the base and the 2′-hydroxyl (OH) group are of major importance in determining configurations of α-anomers and 2′-arabino-β-epimers. For example, hydrogen bonding between the 2′-hydroxyl group and polar centers on the base ring is clearly implicated as a determinant of syn-anti preferences of the purine (adenine) or pyrimidine (uracil) bases in α-nucleoside 3′,5′-cyclic monophosphates. Moreover, barrier heights for interconversion between conformers are sensitive to ribose pucker and 2′-OH orientations. The result clearly show that a change in ribose-ring pucker plays an essential role in relieving repulsive interaction between the base and the 2′-hydroxyl group. Thus a C2′-exo-C3′-endo (₂T³) pucker is favored for α-anomers in contrast with the C4′-exo-C3′-endo (₄T³) from found in β-compounds.     

Design of Peptides Using α,β-Dehydro-residues: Synthesis,Crystal Structure and Molecular Conformation of N-Boc-L-Val-ΔPhe–ΔPhe-L-Ala-OCH3

To obtain general rules of peptide design using α,β-dehydro-residues, a sequence with two consecutive ΔPhe-residues, Boc-L -Val-ΔPhe–ΔPhe- L -Ala-OCH₃, was synthesized by azlactone method in solution phase. The peptide was crystallized from its solution in an acetone/water mixture (70:30) in space group P6₁ with a=b=14.912(3) Å, c= 25.548(5) Å, V=4912.0(6) ų. The structure was determined by direct methods and refined by a full matrix least-squares procedure to an R value of 0.079 for 2891 observed [I?3σ(I)] reflections. The backbone torsion angles ?₁=?54(1)°, ψ₁= 129(1)°, ω₁=?177(1)°, ?₂ =57(1)°, ψ₂=15(1)°, ω₂ =?170(1)°, ?₃=80(1)°, ψ₃ =7(2)°, ω₃=?177(1)°, ?₄ =?108(1)° and ψ^T₄=?34 (1)° suggest that the peptide adopts a folded conformation with two overlapping β-turns of types II and III′. These turns are stabilized by two intramolecular hydrogen bonds between the CO of the Boc group and the NH of ΔPhe³ and the CO of Val¹ and the NH of Ala⁴. The torsion angles of ΔPhe² and ΔPhe³ side chains are similar and indicate that the two ΔPhe residues are essentially planar. The folded molecules form head-to- tail intermolecular hydrogen bonds giving rise to continuous helical columns which run parallel to the c-axis. This structure established the formation of two β-turns of types II and III′ respectively for sequences containing two consecutive ΔPhe residues at (i+2) and (i+3) positions with a branched β-carbon residue at one end of the tetrapeptide.     

Crystal Structure and Conformation of 5‐Fluorouridine: Conformational Preferences for 5‐Fluorinated Pyranosides

Crystals of 5‐fluorouridine (5FUrd) have unit cell dimensions a = 7.716(1), b = 5.861(2), c = 13.041(1)Å, α = γ = 90°, β = 96.70° (1), space group P2₁, Z = 2, ρ_obs = 1.56 gm/c.c and ρ_calc = 1574 gm/c.c The crystal structure was determined with diffractometric data and refined to a final reliability index of 0.042 for the observed 2205 reflections (I ≥ 3σ). The nucleoside has the anti conformation [χ = 53.1(4)°] with the furanose ring in the favorite C2′–endo conformation. The conformation across the sugar exocyclic bond is g⁺, with values of 49.1(4) and ? 69.3(4)° for Φ_θc and Φ_∞ respectively. The pseudorotational amplitude τ_m is 34.5 (2) with a phase angle of 171.6(4)°. The crystal structure is stabilized by a network of N–H…O and O–H…O involving the N3 of the uracil base and the sugar O3′ and O2′ as donors and the O2 and O4 of the uracil base and O3′ oxygen as acceptors respectively. Fluorine is neither involved in the hydrogen bonding nor in the stacking interactions. Our studies of several 5‐fluorinated nucleosides show the following preferred conformational features: 1) the most favored anti conformation for the nucleoside [χ varies from ? 20 to + 60°] 2) an inverse correlation between the glycosyl bond distance and the χ angle 3) a wide variation of conformations of the sugar ranging froni C2′–endo through C3′–endo to C4′–exo 4) the preferred g⁺ across the exocyclic C4′–C5′ bond and 5) no role for the fluorine atom in the hydrogen bonding or base stacking interactions.     

Crystal structure of guanylyl-2′,5′-cytidine dihydrate: An analogue of msDNA-RNA junction in stigmatella aurantiaca

Sequence analysis of msDNA from bacterium such as Stigmatella aurantiaca, Myxococcus xanthus and Escherichia coli B revealed that the guanine residue of the single-stranded RNA is linked to the cytosine residue of the msDNA through a 2′–5′ instead of a conventional 3′–5′ phosphodiester bond. We have now obtained the crystal structure of the self-complementary dimer guanylyl-2′,5′-cytidine (G2′p5′C) that occurs at the msDNA-RNA junction. G2′p5′C crystallizes in the orthorhombic space group P2₁2₁2₁ with a = 8.376(2), b = 16.231(5), c = 18.671(4). CuK ∝ intensity data were collected on a diffractometer in the ω ?2θ scan mode. The amount of 1699 out of 2354 reflections having I ≥ 3σ (F) were considered observed. The structure was solved by direct methods and refined by full-matrix least squares to a R factor of 0.054. The conformation of the guanine base about the glycosyl bond is syn (χ₁ = ?54°) and that of cytosine is anti (χ₂ = 156°). The 5′ and 2′ and ribose moieties show C2′-endo and C3-endo mixed puckering just like in A2′p5′A, A2′p5′C, A2′p5U, and dC3′p5′G. Charge neutralization in G2′p5′C is accomplished through protonation of the cytosine base. An important feature of G2′p5′C is the stacking of guanine on ribose 04′ of cytosine similar to that seen in other 2′–5′ dimers. G2′p5′C, unlike its 3′–5′ isomer, does not form a miniature double helix with the Watson-Crick base-pairing pattern. Comparison of G2′p5′C with A2′p5′C reveals that they are isostructural. A branched trinucleotide model for the msDNA-RNA junction has been postulated. © 1994 John Wiley & Sons, Inc.     

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

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

Correlation between the backbone and side chain conformations in 5′-nucleotides. The concept of a ‘rigid’ nucleotide conformation

Conformational energies of the 5′-adenosine monophosphate have been computed as a function of χ and ψ, of the torsion angles about the side-chain glycosyl C(1′)–N(9) and of the main-chain exocyclic C(4′)–C(5′) bonds by considering nonbonded, torsion, and electrostatic interactions. The two primary modes of sugar puckering, namely, C(2′)-endo and C(3′)-endo have been considered. The results indicate that there is a striking correlation between the conformations about the side-chain glyocsyl bond and the backbone C(4′)–C(5′) bond of the nucleotide unit. It is found that the anti and the Gauche–Gauche (gg), conformations about the glycosyl and the C(4′)–C(5′) bonds, respectively, are energetically the most favored conformations for 5′-adenine nucleotide irrespective of whether the puckering of the ribose is C(2′)-endo or C(3′)-endo. Calculations have also shown that the other common 5′-pyrimidine nucleotides will show similar preferences for the glycosyl and C(4′)–C(5′) bond conformations. These results are in remarkable agreement with the concept of the “rigid” nucleotide unit that has been developed from available data on mononucleotides and dinucleoside monophosphates. It is found that the conformational ‘rigidity’ in 5′-nucleotides compared with that of nucleosides is a consequence of, predominantly, the coulombic interactions between the negatively charged phosphate group and the base. The above result permits one to consider polynucleotide conformations in terms of a “rigid” C(2′)-endo or C(3′)-endo nucleotide unit with the major conformational changes being brought about by rotations about the P–O bonds linking the internucleotide phosphorus atom. IT is predicted that the anti and the gg conformations about the glycosyl and the C(4′)–C(5′) bonds would be strongly preferred in the mononucleotide components of different purine and pyrimidine coenzymes and also in the nucleotide phosphates like adenodine di- and triphosphates.     

The effect of monovalent cations on the association behavior of guanosine 5'-monophosphate, cytidine 5'-monophosphate, and their equimolar mixture in aqueous solution

¹H- and ³¹P-nmr spectroscopy have been used to investigate the self-association of M₂(5′-CMP) [M = Li⁺, Na⁺, K⁺, Rb⁺, or (CH₃)₄ N⁺; 5′-CMP = cytidine 5′-monophosphate], the self-association of Li₂(5′-GMP) (5′-GMP = guanosine 5′-monophosphate), and the heteroassociation of 5′-GMP and 5′-CMP (1 : 1 mole ratio) in aqueous solution as a function of the nature of the monovalent cation. Proton spectral differences for the different 5′-CMP salts exhibit a cation-size dependence and have been ascribed to a change in the stacking geometry. An average stacking association constant of 0.63 ± 0.24M^?1 at 1°C, consistent with the weak stacking interactions of the cytosine bases, was determined for the 5′-CMP salts. Heteroassociation of 5′-GMP and 5′-CMP follows the reverse of the cation order for the formation of ordered aggregates of 5′-GMP. Heteroassociation occurs in the presence of Li⁺, Na⁺, and Rb⁺ ions, but only self-association occurs for the K⁺ nucleotides. Li₂(5′-GMP), which does not form ordered species, self-associates to form disordered base stacks with a stacking constant of 1.63 ± 0.11M^?1 at 1°C.     

Structure Sensitivity of Amino Proton Exchange in 2′ - and 5′ - Guanosine Monophosphate Dianions

Abstract

Proton NMR line broadening methods were used to determine the rates of amino proton exchange for disordered 2′ - and 5′ - GMP dianions in aqueous solutions containing tetramethylammonium (TMA⁺) cations. Replacing TMA⁺ with Na⁺ does not substantially alter the exchange rates, provided that H-bonded, Na⁺-directed tetramer structures are absent. Activation enthalpies (kcal/mol) and entropies (eu) for 2′ - GMP are: ΔH^# = 18.5 ± 1.3, ΔS^# = 9.6 ± 4.2 for theTMA⁺ salt atpH 8.10, and ΔH^# = 14.7 ± 2.6, ΔS^# = -3.7 ± 8.0 for the Na⁺ salt at pH 8.11. Extrapolated values of pseudo first-order rate constants at 25° Care in the range of k = 1–10 sec^?1. At suitable concentrations and temperatures, the Na⁺ salts of both 2′ - and 5′ - GMP formed stacked and unstacked tetramer units. Relative to the exchange kinetics observed for the disordered nucleotide, the exchange process in the tetramer units was catalyzed in half the amino protons and inhibited in the other half. The catalytic process (k < 10³ sec^?3) has been attributed to amino protons not involved in interbase H-bonding, where as the inhibited process (k > 10^?1 sec^?1) was assigned to those protons which do form such bonds. The structure-catalyzed process in both the stacked and unstacked tetramers was manifested by a loss of NMR amino proton intensity due to weighted time-averaging with the resonance for bulk water. A bridging water molecule between an amino proton and a phosphate on an adjacent nucleotide in the tetramer unit may provide a mechanistic pathway for the structure-catalyzed process.     

Structure and Conformation of 1-β-D-Ribo Furanosyl Pyridin-2-one-5-Carboxamide: An Anti-Inflammatory Agent

The pyrimidine nucleoside, 1-β-D-ribofuranosyl pyridine-2-one-5-carboxamide, is an anti inflammatory agent used in the treatment of adjuvant-induced arthritis. It is the 2-one isomer of 1-β-D-ribofuranosyl pyridine-4-one 5-carboxamide, an unusual nucleoside isolated from the urine of patients with chronic myelogenic leukemia and an important cancer marker. Crystals of 1-β-D-ribofuranosyl pyridine-2-one-5-carboxamide are monoclinic, space group C2, with the cell dimensions a = 31.7920(13), b = 4.6872 (3), c = 16.1838(11), β = 93.071(3)°, V = 2408.2(2) ų, D_calc = 1.496 mg/m³ and Z = 8 (two molecules in the asymmetric unit). The structure was obtained by the application of direct methods to diffractometric data and refined to a final R value of 0.050 for 1669 reflections with I ≥ 3σ. The nucleoside exhibits an anti conformation across the glycosidic bond (χ_CN = ?15.5°, ?18.9°), a C3 ′- endo C2 ′ -exo [³ ₂T] ribose pucker and g⁺ across the C(4 ′)-C(5 ′) exocyclic bond. The amino group of the carboxamide group is distal from the 2-one and lacks the intramolecular hydrogen bonding found in the related 2-one molecule. Nuclear magnetic resonance studies shows also an anti conformation across the glycosidic bond but the solution conformation of the furanose ring is not the same as that found in the solid state.