A vibrational spectroscopic study of the self-association of 5′-GMP in aqueous solution

The Raman spectra of highly concentrated solutions of 5′-GMP at neutral and acid pH were recorded in order to better characterize the structure of the self-aggregates formed in these solutions and their melting behavior. Vibrational coupling of the C?O stretching vibrations in tetrameric units at neutral pH is shown to yield a characteristic pattern of two Raman bands at ca. 1730 and 1680 cm^?1 (1708 and 1664 cm^?1 in D₂O), and an iractive mode at 1678 cm^?1 in D₂O. From the intensity of the 1730-cm^?1 band, proportional to tetramer concentration, and that at 1485 cm^?1, which reflects the stacking of the bases, the thermal stability of the self-associates formed at neutral pH is shown to be higher for stacked tetramers. At acid pH, the melting of the helical aggregates responsible for the formation of a gel is preceded by the freeing of the hydrogen-bonded phosphate groups, accompanied by a change of conformation from C3′-endo to C2′-endo in some of the associated ribose units. Previous spectroscopic results suggesting the formation of tetramers as an intermediate step in the melting of the gel were not reproduced in this study.     

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⁺)

     

A vibrational spectroscopic study of the metastable form of associated polyinosinic acid

We have studied by Raman and ir spectroscopy the metastable complex formed by the self-association of polyinosinic acid in aqueous solution. The complex is easily prepared by quickly cooling to ca. 0°C a warm solution of the polyribonucleotide to which a small amount of rubidium salt has been added. Upon heating, this metastable form melts cooperatively near 13°C, well below the dissociation temperature of a stable four-stranded complex, which occurs at 47°C in the same conditions. The presence of several components in the stretching-mode region of the carbonyl groups in the vibrational spectra of the metastable complex suggests that it also has a parallel four-stranded structure. The difference in structure between the two forms is believed to be caused by the presence of fewer metal ions in the central channel of the metastable complex, in agreement with conclusions reached in previous investigations. The Raman spectra further show that the ribose units in the metastable form have a C3′-endo conformation, in contrast with the stable form, for which we have previously suggested a mixed C2′-endo/C3′-endo conformation. © 1996 John Wiley & Sons, Inc.     

Raman spectroscopic elucidation of DNA backbone conformations for poly(dG-dT).poly(dA-dC) and poly(dA-dT).poly(dA-dT) in CsF solution

Raman spectra have been recorded for poly(dG-dT) · poly(dA-dC) and poly(dA-dT) · poly(dA-dT) in low salt and at high concentrations of CsF. Poly(dG-dT) · poly(dA-dC) shows no change in the 682-cm^?1 guanine mode, demonstrating the absence of the Z-structure at high salt. The 790-cm^?1 phosphodiester symmetric stretch, however, shifts up 5 cm^?1 in 4.3M CsF, suggesting a slight conformational change, associated with ion binding or hydration changes. Poly(dA-dT) · poly(dA-dT) shows an additional broad band at 816 cm^?1, attributed to the phosphodiester modes associated with the C3′-endo deoxyribose units in the alternating B-structure. In this case, both the 841- and the 816-cm^?1 asymmetric phosphodiester stretches, associated with the C2′- and C3′-endo units, shift down on addition of CsF in a sequential manner. Correlation of this sequence with that previously observed for the two ³¹P-nmr resonances, establishes that the phosphodiester stretching frequencies depend on the conformation of the 5′-sugar, and not on the 3′-sugar.     

Conformational studies on polynucleotide chains. V. A comparison between the quantum-mechanical and the consistent force field approach

Consistent force field (CFF) calculations were performed for the sugar–phosphate–sugar fragment, taken as a model of the polynucleotide backbone. The potential-energy-function is the sum of four contributions, accounting for bond and angle deformation, torsional motions, and nonbonded interactions. Both deoxyribose and ribose systems, with either C(2′)-endo or C(3′)-endo puckering in the starting geometry of ribose rings, were considered. A fair number of minima of the conformational-energy hypersurface were found. Although the numerical method employed in the CFF context cannot solve the problem of finding the global minimum in a definite way, one of the final conformations has a total energy much more attractive than the others, and may be regarded as the most stable conformation attainable with our potential-energy function. The energy-minimization affects the puckering of the first ribose ring differently from that of the second: in general, for the C(2′)-endo system the second ring retains its starting conformation (Ψ′ = 152°), while in the first the Ψ′ is modified by up to 70°; the opposite occurs for the C(3′)-endo system. This is explained by the different positions of the two rings relative to the phosphate group.     

Spatial configurations of polynucleotide chains. 3. Polydeoxyribonucleotides

The virtual bond scheme set forth in preceding papers for treating the average properties of polyriboadenylic acid (poly rA) is here applied to the calculation of the unperturbed mean-square end-to-end distance of polydeoxyriboadenylic acid (poly dA). The modifications in structure and in charge distribution resulting from the replacement of the hydroxyl group at C_2′ in the ribose residue by hydrogen in deoxyribose produce only minor modifications in the conformational energies associated with the poly dA chain as compared to those found for poly rA. The main difference is manifested in the energy associated with rotations about the C_3′–O_3′ bond of the deoxyribose residue in the C_2′-endo conformation; accessible rotations are confined to the range between 0° and 30° relative to the trans conformation, whereas in the ribose unit the accessible regions comprise two ranges centered at approximately 35° and 85°. The characteristic ratio 〈r²〉0/nl² calculated on the basis of the conformational energy estimates is ≈9 for the poly dA chain with all deoxyribose residues in the C_3′-endo conformation and ≈21 with all residues in the C_2′-endo form. Satisfactory agreement is achieved between the theoretical values and experimental results on apurinic acid by treating the poly dA chain as a random copolymer of C_3′-endo and C_2′-endo conformational isomers present in a ratio of ～1 to 9.     

Molecular conformations and 8-CH exchange rates of purine ribo- and deoxyribonucleotides: investigation by Raman spectroscopy

The rate of deuterium exchange of the 8-CH group in a purine deoxyribonucleotide, is the same as the 8-CH exchange rate in the corresponding purine ribonucleotide, with the exception of 5′-nucleotides of guanine. The observed 20% slower rate of 8-CH exchange in 5′-dGMP versus 5′-rGMP, over the temperature range 50–80°C, are attributable to differences in molecular conformation, including differences in ring puckering of the furanose substituents. Minor differences in 8-CH exhange rates are observed between 5′-and cyclic (3′:5′)-deoxyribonucleotides of a given purine, which are similar to those observed previously between corresponding 5′- and cyclic ribonucleotides that have been attributed to the charge difference of their respective phosphate groups [Ferreira, S. A. & Thomas, G. J., Jr. (1981) J. Raman Spectrosc. 11 , 508–514]. The coupling of guanine and furanose ring structures in the 5′-nucleotides is also evident from the vibrational frequencies of the guanine ring, which are strongly dependent on the pucker of the attached furanose moiety. Raman difference spectroscopy clearly reveals the dependence of purine nucleotide spectra on sugar-ring pucker. In the case of GMP, the guanine characteristic ring breathing mode near 600–700 cm^?1 depends for its exact position and intensity on the proportion of C3′-endo (668 cm^?1) and C2′-endo (682 cm^?1) conformers in equilibrium with one another. The Raman intensity ratio I(668)/I(682) is proposed as a measure of the conformer ratio C3′-endo/C2′-endo in 5′-dGMP with possible application also to nucleic acids. Among cyclic nucleotides, differences in spectra of deoxyribo- and ribo- forms also appear to be related to differences of molecular conformation.     

Conformational analysis of the 2'-deoxyribofuranose ring from proton-proton coupling constants: analysis of a nucleoside-carcinogen adduct formed from 2-acetylaminofluorene utilizing a three-state model

The conformation of the sugar moiety of 8-(N-fluoren-2-ylamino)-2′-deoxyguanosine in solution has been examined as a function of temperature by ¹H-nmr spectroscopy. Analysis of coupling constants shows that lowering the temperature to ?50°C in methanol shifts the conformational equilibrium of the sugar ring resulting in a C2′-endo conformation at a mole fraction of 0.97. The computed phase angle of pseudorotation and amplitude of pucker are 154° and 36°, respectively, with very little discrepancy between the five calculated coupling constants and coupling constants extrapolated from the temperature profiles. A computer program has been written enabling a three-state best-fit analysis. The three-state analysis indicates an equilibrium between C2′-endo, C3′-endo, and 04′-endo conformations. In aqueous solution, the computed mole fraction of the 04′-endo form is 0.18 at 30°C. The conformation associated with the sugar ring and the C4′? C5′ bond is compared to that of 2′-deoxyguanosine.     

Polarized Raman scattering from oriented single microcrystals of d(A5T5)2 and d(pTpT)

Polarized Raman spectra have been obtained from single microcrystals of the duplex of the decamer d(A₅T₅)₂ using a Raman microscope. This is the first report of Raman spectra from a crystal of a deoxyoligomer that contains only long, nonalternating sequences of adenine and thymine. Sequences containing d(A)_n and d(T)_n are of interest in view of recent suggestions that they induce bends in DNA and that they might exist in a nonstandard B-conformation. Polarized Raman spectra of a crystal of d(pTpT) have also been obtained. Both crystals display Raman bands whose intensities are very sensitive to the orientation of the crystal with respect to the direction of polarization of the incident laser beam. These spectra indicate that the helical axes of the oligonucleotides are parallel to the long axes of the crystals and that the d(A₅T₅)₂ is not appreciably bent in the crystal. The Raman spectrum from the d(pTpT) crystal indicates that all of the furanose ring puckers are in a C2′-endo configuration since only the C2′-endo marker band at 835 ± 5 cm^?1 is present. Crystals of d(A₅T₅)₂ show measurable Raman intensities in both the 838- and 816-cm^?1 bands. This indicates the presence of both the C2′-endo and C3′-endo, or possibly other non-C2′-endo, furanose conformations. The 816-cm^?1 band is weak so that only a small fraction of the residues are estimated to be in the non-C2′-endo conformation. In both the d(pTpT) and d(A₅T₅)₂ crystals the intensity of the bands due to vibrations of the backbone show only a small dependence on orientation of the crystals. This result is explained by the low symmetry of the puckered sugar rings. It is concluded that Raman spectra obtained from oligonucleotide crystals in which the orientation of the crystal axes to the laser polarization is not carefully controlled may contain intensity artifacts that are due to polarization effects.     

FT-IR and 1H NMR spectroscopic evidence of sugar ring conformational change in NH4GpG on complexation to form cis-[Pt(NH3)2(GpG)]+

The conformational change of the ribose ring in NH₄GpG and cis-[Pt(NH₃)₂(GpG)]⁺ was confirmed by FT-IR spectroscopic evidence as being C2′-endo, C3′-endo, anti, gg sugar ring pucker in the solid state. These results were compared with ¹H NMR spectral data in aqueous solution. The FT-IR spectrum of NH₄GpG shows marker bands at 802 cm^?1 and 797 cm^?1 which are assigned to the C3′-endo, anti, gg sugar-phosphate vibrations of ribose (?pG) and ribose (Gp?), respectively. The FT-IR spectrum of cis-[Pt(NH₃)₂(GpG)]⁺ (with N7N7 chelation in the GpG sequence) shows a marker band at 800 cm^?1 which is assigned to the C3′-endo, and a new shoulder band at 820 cm^?1 related to a C2′-endo ring pucker. The ribose conformation of (?pG) moiety in NH₄-GpG, C3′-endo, anti, gg changes into C2′-endo, anti, gg when a platinum atom is chelated to N7N7 in the GpG sequence.     

Conformational geometry and vibrational frequencies of nucleic acid chains.

Normal coordinate analysis of diethyl phosphate has been made, which predicts all observed Raman frequencies in the range 170–1300 cm^?1. The force constants from this calculation have been transferred to a vibrational calculation for a simplified model of the backbone of nucleic acids, which also involves the ? O? PO₂^?? O phosphate group and the ? C₅′? C₄′? C₃′? linkage of the ribose. The coordinates of these atoms are those recently given by Arnott and Hukins, which place the ribose ring of B-DNA in a C₃′-exo conformation. This simple polymer model appears to be able to describe adequately the frequency-dependent changes observed in the Raman spectra arising from the backbone vibrations of nucleic acid in going from the B- to A-form. The symmetric ? O? P? O? diester stretch increases in frequency from about 787 cm^?1 in the B-form to 807 cm^?1 in the A-form. The increased frequency characteristic of the A-form is due to the combining of the diester stretch with vibrations involving the C₅′, C₄′, and C₃′ nuclei. The frequency of the symmetric ? O? P? O? diester stretch is shown to be very dependent on the conformation of the ribose ring, indicating that in polynucleotides the ribose ring takes on one of two rigid conformations: C₃′-endo for A-form or C₃′-exo for B-form and “disordered” polynucleotides. The calculation lends confirmation to the atomic coordinates of Arnott and Hukins since the use of other geometries with the same force constants failed to give results in agreement with experimental evidence. The calculations also demonstrate the lowering effect of hydration on the anionic PO stretching frequencies. Experimental results show that the 814-cm^?1 band observed in the spectra of 5′GMP gel arises from a different vibrational mode than that of the 814-cm^?1 band of A-DNA.     

Untenability of the Heteronomous DNA Model for Poly(dA) · Poly(dT) in Solution. This DNA Adopts a Right-Handed B-DNA Duplex in Which the Two Strands are Conformationally Equivalent. A 500 MHz NMR Study Using One Dimensional NOE

Abstract

ID NOE ¹H NMR spectroscopy at 500 MHz was employed to examine the structure of poly(dA)·poly(dT) in solution. NOE experiments were conducted as a function of presaturation pulse length (50, 30, 20 and 10 msec) and.power (19 and 20 db) to distinguish the primary NOEs from spin diffusion. The 10 msec NOE experiments took 49 hrs and over 55,000 scans for each case and the difference spectra were almost free from diffusion.

The spin diffused NOE difference spectra as well as difference NOE spectra in 90% H₂O + 10% D₂O in which TNH3 was presaturated enabled to make a complete assignment of the base and sugar protons. It is shown that poly(dA) ·poly(dT) melts in a fashion in which single stranded bubbles are formed with increasing temperature.

Extremely strong primary NOEs were observed at H2′/H2″ when AH8 and TH6 were presaturated. The observed NOEs at AH2′ and that AH2″ were very similar as were the NOEs at TH2′ and TH2″. The observed NOEs at AH2′ and AH2″when AH8 was presaturated were very similar to those observed at TH2′ and TH2″ when TH6 was presaturated. In addition, presaturation of H1′ of A and T residues resulted in similar NOEs at AH2′/H2″ and TH2′/H2″ region and these NOEs at H2′ and H2″ were distinctly asymmetric as expected in a C2′-endo sugar pucker. There was not a trace of NOE at AH8 and TH6 when AH3′ and TH3′ were presaturated indicating that C3′-endo, × = 30–40° conformation is not valid for this DNA. From these NOE data, chemical shift shielding calculations and stereochemistry based computer modellings, we conclude that poly(dA)·poly(dT) in solution adopts a right- handed B-DNA duplex in which both dA and dT strands are conformationally equivalent with C2′-endo sugar pucker and a glycosyl torsion, ×, of ?73°, the remaining backbone torsion angles being φ′ = 221°, ω′ = 212°, ω = 310°, φ = 149°, ψ = 42°, ψ′ = 139°. The experimental data are in total disagreement with the heteronomous DNA model of Arnott et. al. proposed for the fibrous state. (Arnott, S., Chandrasekaran, R., Hall, I.H., and Puigjaner, L.C., Nucl. Acid Res. 11, 4141, 1983).     

The A and B conformations of DNA and RNA subunits. Potential energy calculations for dGpdC

In order to obtain a molecular picture of the A and B forms of a DNA subunit, potential energy calculations have been made for dGpdC with C(3′)-endo and C(2′)-endo [or C(3′)-exo] sugar puckerings. These are compared with results for GpC. The global minima for dGpdC and GpC are almost identical. They are like A-form duplex DNA and RNA, respectively, with bases anti, the ω′, ω angle pair near 300°, 280°, and sugar pucker C(3′)-endo. For dGpdC, a B-form helical conformer, with sugar pucker C(2′)-endo and ω′ = 257°, ω = 298°, is found only 0.4 kcal/mol above the global minimum. A second low-energy conformation (2.3 kcal/mol) has ω′ = 263°, ω = 158° and ψ near 180°. This has dihedral angles like the original Watson–Crick model of the double helix. In contrast, for GpC, the C(2′)-endo B form is 6.9 kcal/mol above the global minimum. These theoretical results are consistent with experimental studies on DNA and RNA fibers. DNA fibers exist in both A and B forms, while RNA fibers generally assume only the A form. A low-energy conformation unlike the A or B forms was found for both dGpdC and GpC when the sugars were C(3′)-endo. This conformation—ω′,ω near 20°,80°—was not observed for C(2′)-endo dGpdC. Energy surface maps in the ω′,ω plane showed that C(2′)-endo dGpdC has one low-energy valley. It is in the B-form helical region (ω′ ～ 260°, ω ～ 300). When the sugar pucker is C(3′)-endo, dGpdC has two low-energy regions: the A-form helical region and the region with the minimum at ω′ = 16°, ω = 85°.     

Determination of the molecular conformation of beta-D-O2,2'-cyclouridine in aqueous solution by proton magnetic resonance spectroscopy

The solution conformation of β-D -O²,2′-cyclouridine has been determined at 27 and 88°C in D₂O by proton magnetic resonance spectroscopy. The conformation is described in terms of a fixed syn-like sugar-base torsional angle, a type S furanose ring conformation (similar to 2′-endo), and a temperature-dependent exocyclic C(4)′–C(5′) rotamer population containing approximately 50% of the gauche-gauche form at 27°C. β-D -O²,2′-Cyclouridine 5′-phosphate likewise possesses a type S furanose ring conformation.     

The Three-Dimensional Structure of 3′-Deoxycytidine

Abstract

Structural analysis of 3′-deoxycytidine and comparison with 2′-deoxynucleosides reveals no noticeable effect on the conformation of the molecule due to the lack of 3′-oxygen atom. There are two crystallographically independent molecules and both adopt the anti conformation with C3′-endo sugar puckering. A ‘head-to-tail’ packing of the molecules along the b axis results in a virtual ‘2′-5′ polycytidylic acid chain.     

Spectroscopic studies on the structure of poly(8-bromoadenylic acid): Effect of glycosidic torsion angle on the conformation and flexibility in polyribonucleotides

The helix–coil transition and conformational structure of poly(8-bromoadenylic acid) [poly(8BrA)] have been investigated using ¹H- and ¹³C-nmr, CD, and ir spectroscopy. The results have been compared with the structure of the related 5′-mono- and polynucleotides. The chemical shifts of H(2′), H(3′), C(2′), and C(3′) nmr signals show an interesting correlation with both the puckering of ribose ring and glycosidic bond torsion angle. Poly(8BrA) shows an upfield shift of the C(3′) signal and a downfield shift of the H(3′) signal compared to the chemical shifts in poly(A). These shifts are consistent with a C(3′) endo-syn conformation for poly(8BrA). A similar effect has been reported previously and is also observed here on the C(2′) and H(2′) signals when the preferred conformation is C(2′)endo-syn (e.g., in 5′-8BrAMP). The chemical-shift parameters thus act as a probe for studying syn ? anti and N ? S equilibria in solutions. The three-bond ¹H-′¹³C coupling constants between H(1′) and C(8) and C(4) have been measured in poly(8BrA) and 5′-8BrAMP and their structural implications have been discussed. The observed preference of a C(3′)endo-syn conformation for poly(8BrA), coupled with other evidence, throws doubt on the validity of a correlation previously reported whereby a syn conformation is associated with a C(2′)endo ribose pucker. The backbone conformation of randomly coiled poly(8BrA) is very similar to the structures found in polyribonucleotides: poly(A) and poly(U). All three polymers show strong preferences for the backbone angles found in RNA helices. The CD spectrum of poly(8BrA) has a striking relationship to that of poly(A). The signs of all extrema are inverted, and the magnitudes are related by a constant factor. We suggest that these differences result from a change in the angle between coupled transition moment vectors in the two polymers. Infrared spectra of poly(8BrA) in H₂O and D₂O solution are reported for the frequency range below 1400 cm^?1. The antisymmetric >PO stretching vibration is observed at an unusually low frequency in the helix (1214 cm^?1). The symmetric >PO stretch occurs at ～1095 cm^?1 but is not resolved from a ring vibration near this frequency. A conformationally sensitive band, characteristic of helical RNA structures, is observed at 817 cm^?1 and disappears when the helix is melted. This observation confirms the conclusion that ordered poly(8BrA) has a regular helical structure with an RNA backbone conformation. A stereochemical explanation is provided for the failure of poly(8BrA) (or other syn polymers) to form double helices with anti-polyribonucleotides.     

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.     

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.     

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.     

A Raman spectroscopic study on 5′-rGMP gel and self-aggregate

In order to analyze the melting behavior of 5′-rGMP gel at acidic pH and self-aggregate near neutral pH we have obtained Raman spectra of aqueous solutions of 5′-rGMP at various temperatures. At low temperature the intensities of Raman peaks at 502, 585, 1083, 1179, 1322, 1366, 1487, and 1578 cm^?1 decrease due to the formation of ordered structure (Raman hypochromism). In contrast, the peaks at 671, 725, 813, and 1338 cm^?1 become stronger at low temperature (Raman hyperchromism). The Raman hyperchromism of the 671- and 813-cm^?1 peaks have been explained in terms of detailed structural models. Recently, the 668- and 682-cm^?1 peaks in the Raman spectrum of aqueous 5′-rGMP solution have been attributed to the guanine ring breathing vibrations in C3′- and C2′-endo conformers [Benevides, J. B., Lemur, D. & Thomas, G. J., Jr. (1984) Biopolymers 23 , 1011–1024]. On the basis of this information our Raman data can be interpreted to suggest that the continuous helix model of 5′-rGMP gel is right-handed. The 1487-cm^?1 peak intensity has been used to monitor the melting profies at several pHs. Near neutral pH the melting profile shows a single transition, whereas at acidic pH it shows two transitions. From these observations we propose possible pathways for the melting of 5′-rGMP gel formed at acidic pH and self-aggregate formed near neutral pH.