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.     

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⁺)

     

Predicted mode of intercalation of doxorubicin with dinucleotide dimers

Intermolecular molecular mechanics energy calculations have been carried out for doxorubicin interacting with two dinucleotide dimer sequences. The preferred mode of intercalation is in the minor groove with the anthraquinone ring of the drug nearly perpendicular to the base pairs for the (CpG) sequence having alternate C3′ endo-C2′ endo sugar ring puckering. The preferred intercalation conformation of the drug is nearly identical to the N-bromacetyldaunomycin crystal structure. This prediction is qualitatively consistent with the recently reported crystal structure of a d(CpGpCpGpCpG) dimer-daunomycin complex. For the other dinucleotide sequence, (TpC-ApG), minor groove intercalation is also preferred, but the drug conformation can be changed.     

Energetic and structural aspects of ethidium cation intercalation into DNA minihelices

The enthalpy ΔH for the intercalation of the ethidium cation (EC) into DNA minihelices can be decomposed into (1) an energy of conformational adjustment (i.e., the energy of minihelix extension and unwinding from the B-form to the intercalated form) and (2) EC minihelix intermolecular interactions. In the present study, we have focused our attention mainly on a decomposition of the energetic factors of the EC minihelix intermolecular interactions, while the essential features of the energy of conformational adjustment have been discussed in detail elsewhere by us. The structural features of the various resulting energy-minimized EC-intercalated complexes are compared with each other and the initial x-ray model structure. ΔH is estimated to be in the range of ?12.3 to ?24.0 kcal/mol. This theoretical estimate is qualitatively and quantitatively in agreement with a variety of available experimental data. The energy of conformational adjustment is an energetically unfavorable step, while the energetically favorable contribution of the EC minihelix intermolecular interactions is responsible for the overall favorable nature of the intercalation process involving the EC. On the other hand, the observed preference for intercalation into Pyr(3′–5′)Pur DNA sequences over their isomeric Pur(3′–5′)Pyr sequences is controlled by the energy of conformational adjustment and not by the EC minihelix intermolecular interaction contribution. No base-composition effect is expected at EC concentrations normally found at cellular conditions. Moreover, the structural features of the various EC-intercalated complexes are very similar regardless of minihelix base sequence or composition. These results compare favorably with available evidence. The nature of biologically preferred sites of EC binding with the minihelices is discussed.     

Comparative analysis of inosine-substituted duplex DNA by circular dichroism and X-ray crystallography

Leveraging structural biology tools, we report the results of experiments seeking to determine if the different mechanical properties of DNA polymers with base analog substitutions can be attributed, at least in part, to induced changes from classical B-form DNA. The underlying hypothesis is that different inherent bending and twisting flexibilities may characterize non-canonical B-DNA, so that it is inappropriate to interpret mechanical changes caused by base analog substitution as resulting simply from ‘electrostatic’ or ‘base stacking’ influences without considering the larger context of altered helical geometry. Circular dichroism spectra of inosine-substituted oligonucleotides and longer base-substituted DNAs in solution indicated non-canonical helical conformations, with the degree of deviation from a standard B-form geometry depending on the number of I?C pairs. X-ray diffraction of a highly inosine-substituted DNA decamer crystal (eight I?C and two A?T pairs) revealed an A-tract-like conformation with a uniformly narrow minor groove, reduced helical rise, and the majority of sugars adopting a C1′-exo (southeastern) conformation. This contrasts with the standard B-DNA geometry with C2′-endo sugar puckers (south conformation). In contrast, the crystal structure of a decamer with only four I?C pairs has a geometry similar to that of the reference duplex with eight G?C and two A?T pairs. The unique crystal geometry of the inosine-rich duplex is noteworthy given its unusual CD signature in solution and the altered mechanical properties of some inosine-containing DNAs.     

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.     

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.     

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 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.     

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.     

Structure of an 11-mer DNA Duplex Containing the Carbocyclic Nucleotide Analog: 2′-Deoxyaristeromycin

Abstract

2′-deoxyaristeromycin (dAr) is a nucleoside analogue that is resistant to the action of DNA glycosylases. High-resolution NMR spectroscopy and molecular dynamics simulations were used to determine the three-dimensional structure of an 11-mer DNA containing a single dAr?T base pair at its center. Analysis of the spectra revealed the existence of a right-handed duplex in solution, stabilized by Watson-Crick hydrogen bonding and base-stacking interactions. The carbocyclic sugar adopted a C1′-exo conformation and sugars of the 3′-flanking base pair had puckers in the O4′—endo range. The dAr?T base pair was mildly propeller twisted, and the dAr analogue showed a positive roll with the 3′-flanking base. Our findings indicate that the observed resistance of dAr-containing oligodeoxynucleotides to the catalytic action of DNA glycosylases relates to its electronic properties rather than structure, and validate the use of dAr and related carbocyclic nucleoside analogues for biological and structure/function relationship studies.     

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.     

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°.     

Conformational and structural constraints in double-helical polynucleotides

Conformational analysis of antiparallel double-helical polynucleotides with Watson-Crick base pairing was reduced to a four-dimensional problem using original mathematical methods. In the four-dimensional conformational space the family of structures, characterized by the base-pair stacking with the most stable conformations in water solution as well as in the solid state, was localized. For the C′₂-endo sugar pucker, both right-handed and left-handed structures were found; right-handed structures only, however, seem to be allowed for the C′₃-endo pucker, the only possible one for ribonucleotides with base stacking.     

Conformational characteristics of the RNA subunit ApA from energy minimization studies

In an attempt to better our understanding of the conformational stabilities in RNAs, an intensive theoraticl study has been carried out on one of its dimeric subunits, ApA, using an improved set of atom-atom interaction energy parameters and an improved version of energy-minimization technique. The C(3′)0endo and the C(2′)-endo sugar ApA units were sperately considered and 38 probable conformations have been analyzed in each case. The total potential energy, comprising nonbonded, electrostatic, and torsional contributions, was minimized by varying all seven relevant dihedral angles simumtaneously. The result reveal that 17 conformations in the case of C(3′)-endo sugar ApA and 7 confomations in the case of C(2′)-endo sugar ApA unit, the lowest energy conformation corresponds to a nonhelical structure and the A-RNA and the Watson-Crick-yype conformations lie at energy levels of about 0.5 and 1.0 Kcal/mo., respectively, above the lowest energy found. For ApA with the lops of different types in the backbone and they all differ in energies by about 3.5 Kcal/mol with refrence to the lowest energy founs. It is noted that the order ofmprefrence of the base stacking is observed in the A-RNA and the Watson-Crick type conformers. The ApA unit with C(2′)-endo sugar is forced to assume phosphodiester conformations with large deviations fom the expected staggered conformations compared to the ApA unit with C(3′)-endo sugar. The result obtained for ApA are discussed with refrence to those previously obtained for the dApdA unit. Te theoretical predictions are compared with the experimental data on the tRNA^Phe crystal, as well as those on fibrous RNAs and RNa subunitlike crystal structures. This study brings out many important aspects of the conformational stability of ApA which have been missed by studies made by others on this system.     

Conformational characteristics of the trinucleoside diphosphate d(ApApA) from energy-minimization studies

Energy-minimization studies were carried out on the trinucleoside diphosphate d(ApApA). The potential energy contributions from nonbonded, electrostatic, hydrogen-bonding, and torsional interactions were minimized by treating the 13 relevant dihedral angles as simultaneous variables. For the C(3′)-endo trimer, 14 low-energy conformations are within 10 kcal/mol above the lowest energy found, compared to only 3 in the case of the C(2′)-endo trimer. This result shows the flexible character of the C(3′)-endo unit. The hairpin-type, loop-promoting conformer with (ω′,ω) = (101°, 59°) was found to be the most favored structure at the 3′-terminus of d(ApApA). The predicted U- and L-type bend conformers were found to lie within 5 kcal/mol, compared to the lowest energy B-DNA structure. The A-DNA and Watson-Crick DNA types of helical conformers also lie within very small energy barriers. The phosphate group at the 5′-end of the nucleotide residue has a definite influence on the base of the corresponding nucleotide, keeping it in the normal anti-region, and hence on the base-stacking property. The results are compared with the presently available experimental data, mainly with the tRNA^Phe crystal.     

Correlation between sugar pucker and the orientation around the C3′?O3′ bond (Φ′) in 3′-mononucleotides

Classical potential functions (CPF) calculations on 3′-mononucleotides, the building blocks of nucleic acids, predict a correlation between the sugar ring pucker and the torsion angle Φ′ around the C3′? O3′ bond. In ribonucleotides, the value of Φ′ depends on the sugar pucker, viz. the C2′-endo sugar pucker is associated with Φ′ = 210° and 270°, while the C3′-endo sugar pucker favors only Φ′ = 210°. On the other hand, in deoxyribonucleotides, both sugar puckers show a preference for Φ′ = 180°. These theoretical predictions are fully corroborated by the results obtained from x-ray and nmr studies on mono-, di-, and polynucleotides.     

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.     

SYNTHESIS,STRUCTURE, AND CONFORMATION OF ANTI-TUMOR AGENTS IN THE SOLID AND SOLUTION STATES: HYDROXYL DERIVATIVES OF FTORAFUR

ABSTRACT

The pyrimidine antimetabolite Ftorafur [FT; 5-fluoro-1-(tetrahydro-2-furyl)uracil] has shown significant antitumor activity in several adenocarcinomas with a spectrum of activity similar to, but less toxic than, 5-fluorouracil (5-FU). It is considered as a prodrug that acts as a depot form of 5-FU, and hence the two drugs exhibit a similar spectrum ofchemotherapeutic activity. Ftorafur is metabolized in animals and humans when hydroxyl groups are introduced into the tetrahydrofuran moiety. These metabolites are also thought to be as active as ftorafur but less toxic than 5-FU. Hydroxyl derivatives: 2′-hydroxyftorafur (III), 3′-hydroxyftorafur (IV) and 2′,3′-dihydroxyftorafur (II) were synthesized and X-ray and NMR studies of these hydroxyl derivatives were undertaken in our laboratories to study the structural and conformational features of Ftorafur and its metabolites in the solid and solution states. X-ray crystallographic investigations were carried out with data collected on a CAD-4 diffractometer. The structures were solved and refined using the SDP crystallographic package of Enraf-Nonius on PDP 11/34 and Microvax computers. All of the compounds studied had the base in the anti conformation. The glycosidic torsion angles varied from ?20 to 60 degrees. There is an inverse correlation between the glycosyl bond distances and the χ angle. Molecules with a lower χ angle have a larger bond distance and vice versa. The sugar rings show a wide variation of conformations ranging from C2′-endo through C3′-endo to C4′-exo. The crystal structures are stabilized by hydrogen bonds involving the base nitrogen atom N3 and the hydroxyl oxygen atoms of the sugar rings as donors and the keto oxygens O2 and O4 of the base and the hydroxyl oxygen atoms O2′ and O3′ as acceptors. The NMR studies were carried out on Brüker 400 and 600 MHz instruments. Simulated proton spectra were obtained through Laocoon, and pseudorotational parameters were solved by Pseurot. Presence of syn or anti forms was demonstrated with the use of NOE experiments. The glycosyl conformations in solution vary more widely than in the solid state. The conformations of the sugar molecules are in agreement with the values obtained in the solid state. The studies of the structure and conformation in the solid and solution states give a model for the Ftorafur molecule that could be used in structure, function and biological activity correlation studies.     

The crystal structure of an alternating RNA heptamer r(GUAUACA) forming a six base-paired duplex with 3'-end adenine overhangs

The crystal structure of an alternating RNA heptamer r(GUAUACA) has been determined to 2.0 Å resolution and refined to an R_work of 17.1% and R_free of 18.5% using 2797 reflections. The heptamer crystallized in the space group C222 with a unit cell of a = 25.74, b = 106.58, c = 30.26 Å and two independent strands in the asymmetric unit. Each heptamer forms a duplex with its symmetry-related strand and each duplex contains six Watson–Crick base pairs and 3′-end adenosine overhangs. Therefore, two kinds of duplex (duplex 1 and duplex 2) are formed. Duplexes 1 stack on each other forming a pseudo-continuous column, which is typical of the RNA packing mode, while duplex 2 is typical of A-DNA packing with its termini in abutting interactions. Overhang adenine residues stack within the duplexes with C3′-endo sugar pucker and C2′-endo sugar pucker in duplexes 1 and 2, respectively. A Na⁺ ion in the crystal lattice is water bridged to two N1 atoms of symmetry-related A7 bases.