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⁺)

     

Conformations of cyclic 2,3-nucleotides and 2,3-Cyclic-5-diphosphates. Interrelation between the phase angle of pseudorotation of the sugar and the torsions about the glycosyl C(1)-N and the backbone C(4)-C(5) bonds

Semiempirical potential energy calculations have been carried out for cyclic 2′,3′-nucleotides and their 5′-phosphorylated derivatives, which are the intermediates in the hydrolysis of RNA. Calculations have been performed for both purine and pyrimidine bases for the observed O(1′)-endo, O(1′)-exo and the unpuckered planar sugar ring conformations. It is found that the mode of sugar pucker largely determines the preferred conformations of these molecules. For cyclic 2′,3′-nucleotides themselves, the O(1′)-endo sugars show a preference for the syn glycosyl conformation while the O(1′)-exo sugars exclusively favor the anti conformation regardless of whether the base is a purine or pyrimidine. For the unpuckered planar sugar, the syn conformation is favored for purines and anti for pyrimidines. Both the gauche (+) (60°) and trans (180°) conformations about the C(4′)? C(5′) bond are favored for O(1′)-endo sugars, while the gauche (?) (300°) and trans (180°) are favored for O(1′)-exo sugars. On the contrary, the 5′-phosphorylated cyclic 2′,3′-nucleotides of both purines and pyrimidines show a preference for the anti-gauche (+) conformational combination about the glycosyl and C(4′)? C(5′) bonds for the O(1′)-endo sugars and the anti-trans combination for the O(1′)-exo sugars. The correlation between the phase angle of the sugar ring and the favored torsions about the glycosyl and the backbone C(4′)? C(5′) bonds as one traverses along the pseudorotational pathway of the sugar ring is examined.     

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°.     

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.     

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.     

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.     

A vibrational spectroscopic study of the self-association of polyinosinic acid and polyguanylic acid in aqueous solution

We have studied by Raman and ir spectroscopy the structure of self-associated polyinosinic acid and polyguanylic acid in aqueous solution. The results are consistent with the formation of a four-stranded complex, which melts cooperatively near 60°C in the case of poly (I) in the presence of K⁺ ions. The conformation of the ribose in both systems is mixed C2′-endo/C3′-endo, giving a structure that is intermediate between the extremes proposed previously from x-ray diffraction studies. Characteristic Raman bands for the C2′-endo ribose conformation in polyribonucleotides are identified. The four-stranded structure of poly (I) appears to be very flexible, with ≈15% of the tetrameric segments being disrupted and ≈30% of the ribose units adopting a disordered conformation prior to melting. This disordering process increases to ≈75% above the melting transition, with the remaining ≈25% of the ribose units keeping an ordered C2′-endo or C3′-endo conformation. © 1994 John Wiley & Sons, Inc.     

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.     

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.     

Interaction of molecules with nucleic acids. II. Two pairs of families of intercalation sites, unwinding angles, and the neighbor-exclusion principle

Intercalation-site geometries are generated for a tetramer duplex extracted from B-DNA. Glycosidic angles and puckers of the deoxyribose sugar groups bonded to base pairs BP₁ and BP₄, namely, those at either end of the tetramer duplex, are assumed to be those of B-DNA to insure continuity. All possible geometrical conformations for combinations of C(2′)-endo, C(3′)-endo, C(2′)-exo, and C(3′)-exo sugar puckers are determined for the tetranucleotide backbone. Those with minimum energy are selected as candidates for intercalation sites. Calculations reveal two pairs of physically meaningful families of intercalation sites which occur in two distinct regions, I and II, of helical angles which orient BP₂ relative to BP₃ and with the helical axis disjointed between these base pairs. For each site I and II within BP₂ and BP₃, there are two distinct backbone conformations, A and B, connecting BP₃ to BP₄ or BP₁ to BP₂ which do not disrupt backbone conformations connecting BP₂ to BP₃. Hence two pairs, IA and IB, and IIA and IIB, of intercalation sites exist in which the sugar puckers along the backbone of the tetramer alternate from C(2′)-endo to C(3′)-endo on the backbone (5′p3′) connecting BP₂ to BP₃. The glycosidic angles of the C(3′)-endo sugar χ₃^γ are, coincidentally, 80° ± 2° for both conformations γ = A and B connecting BP₃ to BP₄ along the phosphate backbone (5′p3′). Consistent with the theoretical results, the experimental unwinding angles can be grouped into two categories with absolute values of 18° and 26°. The theoretical unwinding angles for sites IA and IB of 16° and for sites IIA and IIB of 20° occur for a displacement of -0.8 Å in the helical axes of BP₂ and BP₃ and for a 100% G·C composition, with a decrease depending on the amount of A·T base pairs present. Ratios of theoretical unwinding angles of sites I and II, which range from 0.75 to 0.84 for the two principal sites, compare well with the experimental value of 0.71. The theoretical results, in agreement with experimental observation, provide a new interpretation of the nature and conformation of the possible binding sites. Conformations obtained from these studies of intercalation sites in a tetramer duplex are used to rationalize the well-known neighbor-exclusion principle. The possibility of violation of this principle is demonstrated by the existence of two families of physically meaningful conformations. Conformations of unconstrained dimer duplexes are also obtained, one of which corresponds to the experimental crystal structure of ethidium–dinucleoside complexes, but these cannot be joined to the B-DNA structure. Backbone conformations of the tetramer duplex can be constructed until the base-pair separation reaches 8.25 Å, which may limit the molecules that can intercalate.     

Conformational studies on polynucleotide chains. III. Intramolecular energy maps and comparison with experiments

Conformational energy maps for the four combinations of two consecutive torsional angles of the backbone structure of polydeoxyribonucleotides are presented. Both the C(2′)-endo and the C(3′)-endo conformation of sugar rings were considered. The energies were evaluated with an analytical expression representing the best fit to ab initio energies computed in the Hartree-Fock approximation, and consisting of a contribution from nonbonded interactions of the Lennard-Jones 6-12 type and an intrinsic torsional potential. It is shown that the minima of these maps are in excellent agreement with the most stable conformations as obtained from x-ray crystallographic analysis of nucleic acids and polynucleotides.     

Molecular and crystal structure of an intercalation complex: Proflavine–cytidylyl-(3′,5′)-guanosine

The high-resolution crystal and molecular structure of a 3:2 complex of proflavine and cytidylyl-(3′,5′)-guanosine is described. The complex exhibits more than one mode of dye binding to the dinucleoside phosphate. One proflavine cation is symmetrically intercalated between the base pairs. The other proflavine cations and ones related by symmetry stack above and below the base pairs and also hydrogen bond externally to the duplex. The conformation of the CpG is most similar to A-RNA with all C(3′)-endo sugar puckering. To allow the base pairs to stretch from the normal 3.4-Å separation to a 6.8-Å separation, the torsion angles ? and χ of the guanosine are increased by about 60° from the values found in RNA. The crystal structure itself contains disordered sulfate anions and is highly solvated, with all but one water molecule involved in a continuous water–sulfate channel.     

Flexibility of the furanose ring in nucleic acids: a compilation of crystal data

A compilation of crystal structure data on deoxyribo- and ribonucleosides and their higher derivatives is presented. The aim of this paper is to highlight the flexibility of deoxyribose and ribose rings. So far, the conformational parameters of nucleic acids constituents of ribose and deoxyribose have not been analysed separately. This paper aims to correlate the conformational parameters with the nature and puckering of the sugar. Deoxyribose puckering occurs in the C2′ endo region while ribose puckering is observed both in the C3′ endo and C2′ endo regions. A few endocyclic and exocyclic bond angles depend on the puckering and the nature of the sugar. The majority of structures have an anti conformation about the glycosyl bond. There appears to be a puckering dependence on the torsion angle about the C4′C5′ bonds. Such stereochemical information is useful in model building studies of polynucleotides and nucleic acids.     

Molecular structure of 2,2′-anhydro-1-β-D-arabinofuranosyl cytosine hydrochloride (cyclo ARA-C): A highly rigid nucleoside

The molecular structure of cyclo ara-C hydrochloride has been determined by x-ray diffraction methods. The ether linkage between the base and sugar moieties severely restricts the conformation about the glycosyl bond and the mode of sugar puckering. The glycosyl torsion angle (X_CN =299°) lies in a region outside the $\text{anti}\text{and}\text{syn}$ ranges found for the β-nucleosides. The arabinose ring exhibits C(4′)-endo (⁴E) mode of puckering, with a pseudorotation phase angle P of 233°. The positive charge on the base apparently stabilizes the $\text{gauche}\text{-}\text{gauche}$ conformation of the C(5′)-O(5′) bond despite the short contacts between O(5′) and C(2) and N(1) of the base.     

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.     

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.     

Cytldlne Cyclic (3′, 5′) Monophosphate: Cyclic Nucleotide With a Non-Characteristic Ribose Ring Conformation

Abstract

Cytidine 3′,-5′-cyclic phosphate (cCMP) occurs in nature and has growth stimulatory activity on L-1210 cells. The initiation of cell growth by cCMP, under conditions where CAMP, cGMP and cUMP delay the onset of proliferation suggests that cCMP may play a regulatory role in the cell metabolism. It has been reported that in 3′,5′-cyclic nucleotides, the phosphate ring fused to the furanose ring resuicts the conformation of the furanose ring to the twist form C(3′) endo C(4′) exo (³T₄), in contrast to the C(2′) endo C(3′) endo (²T₃) and C(3′) endo C(2′) exo (³T₂) twist forms normally found in nucleotides and nucleosides. We have carried out an accurate crystal structure of cCMP and found that the furanose ring in cCMP has the C(3′) endo C(2′) exo conformation (³T₂), with a pseudo rotation amplitude (P) of 44° and phase angle τ_m of 12°. cCMP is in low anti conformation (X_CN = 15.4°) and O(5′) has the fixed g conformation. The phosphate ring is constrained to the chair conformation, as in other cyclic nucleotides. The two exocyclic P-O bond distances are short (1.489, 1.476Å) and the ring angle at N(3) is large (125.2°) suggesting that the molecule in the solid state is a zwitterion with a plus charge on N(3). The crystals are hydrated and highly unstable. The three water molecules are highly disordered in ten locations. The crystals of cCMP 3H₂O are hexagonal, a = 16.294(3), b = c = 11.099(4)Å, space group P6₁, final R value is 0.067 for 1620 reflections 230.     

Visualization of drug--nucleic acid interactions at atomic resolution. V. Structure of two aminoacridine--dinucleoside monophosphate crystalline complexes, proflavine--5-iodocytidylyl (3'-5') guanosine and acridine orange--5-iodocytidylyl (3'-5') guanosine

Acridine orange and proflavine form complexes with the dinucleoside monophosphate, 5-iodocytidylyl(3′–5′)guanosine. The acridine orange-iodoCpG² crystals are monoclinic, space group P2₁, with unit cell dimensions $\text{a = 14.36}\text{A}\text{?}\text{, b = 19.64}\text{A}\text{?}\text{, c = 20.67}\text{A}\text{?}$, β = 102.5 °. The proflavine-iodoCpG crystals are monoclinic, space group C2, with unit cell dimensions $\text{a = 32.14}\text{A}\text{?}\text{, b = 22.23}\text{A}\text{?}\text{, c = 18.42}\text{A}\text{?}$, β = 123.3 °. Both structures have been solved to atomic resolution by Patterson and Fourier methods, and refined by full matrix least-squares.Acridine orange forms an intercalative structure with iodoCpG in much the same manner as ethidium, ellipticine and 3,5,6,8-tetramethyl-N-methyl phenanthrolinium (Jain et al., 1977, Jain et al., 1979), except that the acridine nucleus lies asymmetrically in the intercalation site. This asymmetric intercalation is accompanied by a sliding of base-pairs upon the acridine nucleus and is similar to that observed with the 9-aminoacridine-iodoCpG asymmetric intercalative binding mode described in the previous papers (Sakore et al., 1977, Sakore et al., 1979). Basepairs above and below the drug are separated by about 6.8 Å and are twisted about 10 °; this reflects the mixed sugar puckering pattern observed in the sugar-phospate chains: C3′ endo (3′–5′) C2′ endo (i.e. each cytidine residue has a C3′ endo sugar comformation, while each guanosine residue has a C2′ endo sugar conformation), alterations in glycosidic torsional angles and other small but significant conformational changes in the sugar-phosphate backbone.Proflavine, on the other hand, demonstrates symmetric intercalation with iodoCpG. Hydrogen bonds connect amino groups on proflavine with phosphate oxygen atoms on the dinucleotide. In contrast to the acridine orange structure, base-pairs above and below the intercalative proflavine molecule are twisted about 36 °. The altered magnitude of this angular twist reflects the sugar puckering pattern that is observed: C3′ endo (3′–5′) C3′ endo. Since proflavine is known to unwind DNA in much the same manner as ethidium and acridine orange (Waring, 1970), one cannot use the information from this model system to understand how proflavine binds to DNA (it is possible, for example, that hydrogen bonding observed between proflavine and iodoCpG alters the intercalative geometry in this model system).Instead, we propose a model for proflavine-DNA binding in which proflavine lies asymmetrically in the intercalation site (characterized by the C3′ endo (3′–5′) C2′ endo mixed sugar puckering pattern) and forms only one hydrogen bond to a neighboring phosphate oxygen atom. Our model for proflavine-DNA binding, therefore, is very similar to our acridine orange-DNA binding model. We will describe these models in detail in this paper.     

Crystal Structure and Molecular Conformation of 4-Thiouracil-2′-Trifluorothioacetamide -3′, 5′-Diacetyl-β-D-Riboside

Abstract

4-thiouracil-2′-trifluorothioacetamide-3′, 5′-diacetyl-β-D-riboside is one of the modified thiouracil analogs synthesized in our institute. The determination of the crystal and molecular structure of this compound was carried out with a view to study the conformation of the molecule in the solid state as well as to investigate the conformations of the trifluoroacetamide and the acetyl substituents of the ribose and their effects on the conformation of the ribose ring. Crystals of 4-thiouracil-2′-trifluorothioacetamide-3′,5′- diacetyl-β-D-riboside are orthorhombic, space group P2₁ 2₁ 2₁, with cell dimensions a= 15.351 (2), b= 15.535 (1), c= 8.307 (1) Å, V=1981.0 (7) ų, Z=4, D_m= 1.53, D_c=1.527 g/c.c. and μ=30.1cm -¹. The structure was determined using CuKα (λ, =1.5418 Å) at a temperature T of 297K, with 2333 reflections, which were collected on a Enraf-Nonius CAD-4 diffactometer, out of which 2249 (I ≥20) were considered observed. The structure was determined by direct methods using MULTAN and refined by full matrix least squares method to a final reliability factor of 0.054 and a weighted R factor of 0.079. The nucleoside is in the anti conformation [X_CN =51.4 (5)°], the ribose has the unusual C (2′) endo -C (1′) exo (²T₁), and a g+ conformation [ψ=47.5 (4)] across C(4′)-C(5′) bond. The pseudorotation angle P is 152.8 (4) ° and the amplitude of pucker τ_m of 42.7 (3)°. The average C-F bond distance is 1.308 Å. There is no base pairing and the typical base-base hydrogen bonded interactions are not present in this structure. On the other hand, a hydrogen bonded dimer is formed involving C(3′) - H(3′)… O (2) and N(3) -H (N3) … O (Al) hydrogen bonds joining the base, ribose ring and the acetyl group. The trend towards longer exocyclic bonds at the acetyl centers in compounds with strongly electronegative aglycones, is also exhibited in this compound, with C(3′)-O(3′) and C(5′)-0(5′) being much longer than C(1′)-O(4′). The acetyl groups also take part in C-H…O hydrogen bonding with the acetyl oxygen atom OA2.     

1H-, 13C-, 31P-NMR studies and conformational analysis of NADP+, NADPH coenzymes and of dimers from electrochemical reduction of NADP+

All H,H, H,P and several C,P coupling constants, including those between C-4′ and the vicinal phosphorus atom, have been determined for NADP⁺, NADPH coenzymes and for a 4,4-dimer obtained from one-electron electrochemical reduction of NADP⁺. From these data the preferred conformation of the ribose, that of the 1,4-dihydronicotinamide rings, and the conformation about bonds C(4′)C(5′) and C(5′)O(5′) were deduced. The preferred form of the 1,4- and 1,6-dihydropyridine rings and the conformation about the ring-ring junction were also obtained for all the other 4,4- and 4,6-dimers formed in the same reduction. All the dimers show a puckered structure, i.e., a boat form for the 1,4- and a twist-boat for the 1,6-dihydronicotinamide ring; both protons at the ring-ring junctions are equatorial and have preferred gauche orientation. On the contrary, the reduced coenzyme NADPH displays a planar or highly flexible conformation, rapidly flipping between two limiting boat structures. The conformation of the ribose rings, already suggested for the NADP coenzymes to be an equilibrium mixture of C(2′)-endo (S-type) and C(3′)-endo (N-type) puckering modes, has been reexamined by using the Altona procedure and the relative proportion of the two modes has been obtained. The S and N families of conformers have almost equal population for the adenine-ribose, whereas for the nicotinamide-ribose rings the S-type reaches the 90%. The rotation about the ester bond C(5′)O(5′) and about C(4′)C(5′), defined by torsion angles β and γ respectively, displays a constant high preference for the trans conformer β^t (75–80%), whereas the rotamers γ are spread out in a range of different populations. The values are distributed between the gauche γ⁺ (48–69%) and the rans γ^t forms (28–73%). The γ⁺ conformer reaches a 90% values in the case of NADP⁺ and NMN⁺. The conformations of the mononucleotides 5′-AMP, NMN⁺ and NMNH were also calculated from the experimental coupling constant values of the literature.