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.     

X-Pro peptides. A theoretical study of the hydrogen bonded conformations of (α-aminoisobutyryl-l-prolyl)n sequences

Intramolecularly hydrogen bonded conformations of (Aib-Pro)_n sequences have been analysed theoretically. Both 4→1 (C₁₀ and 3→1 (C₇ hydrogen bonded regular structures are shown to be stereochemically feasible. Conformational energies for the helical structures have been estimated using classical potential energy methods. Both C₁₀ and C₇ conformations have very similar energies. Pyrrolidine ring puckering has a pronounced effect on the energies, and only Cγ-endo puckered Pro residues can be accommodated. The theoretical calculations using spectroscopic data suggest that the recently proposed novel 3₁₀ helical conformation for benzyloxycarbonyl(Aib-Pro)₄-methyl ester is in solution, is indeed energetically and stereochemically favourable.     

A UV resonance Raman investigation of poly(rI): Evidence for cation-dependent structural perturbations

Poly(rI) stabilized by either Na⁺ or K⁺ was investigated using uv resonance Raman (UVRR) spectroscopy. Raman excitation profiles of inosine 5′-monophosphate demonstrated the 250 nm excitation selectively enhances base stacking interactions, while ribose and carbonyl stretching vibrations are preferentially enhanced with 210 nm excitation. These wavelengths were used to examine the structure of poly(rI) in the presence of either K⁺ or Na⁺ as a function of temperature. UVRR studies revealed that the K⁺ stabilized form is more thermally stable, yielding a T_m of ∼ 47°C compared to a T_m of ∼ 30°C for the Na⁺ stabilized form. We observed that both the ribosyl conformation and the coordination of the carbonyl groups depend on the nature of the cation. The C₆O stretching frequency indicates that Na⁺ coordinates much more strongly to the carbonyl groups than K⁺ (1672 cm⁻¹ Na⁺ vs 1684 cm⁻¹ K⁺ at 4°C). Conformationally sensitive modes of the phosphate backbone and the ribosyl ring indicate that Na⁺ stabilized poly(rI) predominantly exists in a C_3′-endo ribose conformation, whereas K⁺ stabilized poly(rI) adopts a C_2′-endo conformation possibly as a consequence of the larger ionic radius of the K⁺ ion. © 1998 John Wiley & Sons, Inc. Biopoly 46: 475–487, 1998     

Structural and Conformational Studies on Deoxyguanosyl-3′,5′-Deoxyadenosine Monophosphate and Its Ethyl Phosphotriester Analogs - Left-Handed Dimers

Abstract

The mode of base-base stacking, the handedness and the sugar(dGpA)phosphate backbone conformation of deoxyguanosyl 3′-5′ deoxyadenosine and its diastereomeric ethyl phosphotriester analogs were studied by ¹H NMR, UV and CD spectroscopy. The results indicate the three dimers are left-handed, while the sugar phosphate backbone is comprised predominantly of C_2′-endo, gg (C_4′-C_5′) and g′g′ (C_5′-O) conformers. The two bases are extensively stacked and interact about 90° along the dyad axes. The extent of base overlap in dGpA is slightly greater than in either ethyl phosphotriester analog. The absolute configurations of the two ethyl phosphotriester diastereoisomers of dGpA can be assigned by one-dimensional and two-dimensional ¹H NMR nuclear Overhauser enhancement experiments.     

Conformation of the common purine (β) ribosides in solution: further evidence for a correlation between N-S state of the ribose moiety and syn-anti equilibrium

The solution conformations of adenosine, guanosine and inosine in liquid ND₃ have been determined by NMR. Comparison of the Karplus analysis of the proton HR spectra of the ribose moiety obtained in this solvent with the data from aqueous solutions of A and I proves that the conformations of the nucleosides are very similar in both liquids. From the analysis of the vicinal coupling constants of the ring protons it has been deduced that the S state C(2′)-endo is slightly preferred. The mole fraction in S approximates 0.6 for all three nucleosides. C-13 relaxation measurements have been applied in the determination of the correlation times for rotational diffusion. Only at temperatures below −40‡ C is the pseudorotation of the furanoside ring slowed down sufficiently for it not to contribute to the measured relaxation rates. From NOE studies and T¹ measurements on the individual protons it is derived that the N, C(3′)-endo, form of the ribose is correlated with an anti conformation of the base (Y≈210‡ to 220‡) and the S, C(2′)-endo, form of the ribose with a syn conformation of the base (Y≈30‡ to 50‡). The glycosyl torsion angles derived for the two conformations of A, G, and I are equal within the limits of accuracy.     

Conformation Analysis of Two Anti-HIV Nucleoside Analogues 2′,3′-Dideoxy-3′-fluorocytidine and Its N4-Dimethylaminomethylene Prodrug Derivative

Abstract

Crystal structure analysis of 2′,3′-dideoxy-3′-fluorocytidine (1) and its prodrug derivative, N⁴-dimethylaminomethylene-2′,3′-dideoxy-3′-fluorocytidine (2), active anti-HIV nucleoside analogues, reveals that both structures adopt an anti conformation about the glycosyl bond. The furanose ring is C2′-endo for (2) and C2′-endo/C1′-exo and C2′-endo/C3′-exo for the two independent molecules of (1), respectively.     

Preparation and crystal structure of the hydroxo-bridged complex biscyclo-tri-μ-hydroxo-tris[(trans-1,2-diaminocyclohexane)platinum(II)] tris

The title compound, [C₁₈H₄₅N₆O₃Pt₃]2(SO₄)₃·14H₂O, belongs to space group C2/c, with a = 25.90(2) Å, b = 14.33(2) Å, c = 23.74(3) Å, β = 122.88(7)°, and Z = 4. The structure was refined on 2899 independent nonzero reflections to an R factor of 0.042. The crystal contains hydroxobridged cyclic [Pt₃(OH)₃(C₆H₁₄N₂)₃]³⁺ ions, in which the Pt₃O₃, ring has a chair conformation. The coordination around each Pt atom is square planar and the cyclohexyl ring lies roughly in the same plane. A large cavity between two trimeric ions related by a twofold axis is filled with one SO₄^2- ion and five water molecules, which participate in an intricate network of hydrogen bonds among themselves and with the hydroxo and amino groups of the complex cation. These units are held together in the crystal by stacking interactions between Pt(OH)₂(C₆H₁₄N₂) “planes” belonging to adjacent molecules, as well as by hydrogen bonds involving the remaining SO₄^2- ions and water molecules. The presence of the cyclohexane ring precludes λ-δ interconversion in the chelate ring and imparts rigidity to the Pt(trans-dach)²⁺ unit.     

Prediction of electrocatalytic activity of some nitrogen-doped polyaromatic hydrocarbons by molecular modelling

Density function theory calculations of minimum energy structure of an oxygen molecule and oxygen atom bonded to the two dimensional molecules, C₂₃NH₁₂, coronene and C₂₁NH₁₄, pentacene doped with nitrogen, indicate the structures are at a minimum on the potential energy surface having no imaginary frequencies. Calculation of the bond dissociation energy (BDE) to remove an oxygen atom from nitrogen-doped pentacene to which is bonded O₂, (C₂₁NH₁₄O₂) shows it is less than that to dissociate O₂. However, this is not the case for nitrogen-doped coronene. This suggests that nitrogen-doped pentacene could be an effective catalyst for the oxygen reduction reaction in fuel cells assuming it is O₂ dissociation. It is also shown that O₂H can bond to nitrogen-doped coronene and pentacene and that the BDE to remove OH is less than that to remove OH from O₂H indicating that N-doped coronene and pentacene could also catalyse this reaction. The calculated adsorption energy for O₂ and O₂H on these molecules is negative indicating they can bond to N-doped coronene and pentacene.     

Coordination chemistry of anticrowns: Synthesis and X-ray crystal structure determination of the polydecker sandwich complexes of cyclic trimeric perfluoro-o-phenylenemercury with azulene and 6-(N,N-dimethylamino)pentafulvene

The interaction of cyclic trimeric perfluoro-o-phenylenemercury (o-C₆F₄Hg)₃ (1) with azulene results in the formation of a complex, {[(o-C₆F₄Hg)₃](azulene)} (2), containing one molecule of azulene per one macrocycle molecule. The complex represents a polydecker sandwich wherein the azulene units alternate with the molecules of the mercury anticrown. The reaction of 1 with 6-(N,N-dimethylamino)pentafulvene (DMAPF) also gives a 1:1 complex, {[(o-C₆F₄Hg)₃](DMAPF)} (3), having a polydecker sandwich structure in the crystal. In complex 2, both the C₅ and C₇ rings of the azulene ligand are involved in the bonding to the Hg sites of 1. In complex 3, the C₅ ring of the fulvene ligand together with its exocyclic carbon atom take part in the coordination to the mercury centres. In both adducts, the negatively charged five-membered ring of the azulene and, correspondingly, the fulvene moieties is arranged in the space between the central Hg₃C₆ rings of the adjacent macrocycles while the remaining portion of these moieties is disposed outside this space. The molecules of azulene and DMAPF in 2 and 3 are bonded to 1 through donation of their π-electrons on vacant orbitals of the Hg atoms. The synthesized 2 and 3 are the first examples of structurally characterized complexes of azulene and DMAPF with a non-transition metal compound.     

Computer Modelling Studies on the Mechanism of Action of Ribonuclease T1

Abstract

The mechanism of action of ribonuclease (RNase) T₁ is still a matter of considerable debate as the results of x-ray, 2-D nmr and site-directed mutagenesis studies disagree regarding the role of the catalytically important residues. Hence computer modelling studies were carried out by energy minimisation of the complexes of RNase T₁ and some of its mutants (His40Ala, His40Lys, and Glu58Ala) with the substrate guanyl cytosine (GpC), and of native RNase T₁ with the reaction intermediate guanosine 2′, 3′-cyclic phosphate (G>p). The puckering of the guanosine ribose moiety in the minimum energy conformer of the RNase T₁ - GpC (substrate) complex was found to be O4′-endo and not C3′-endo as in the RNase T₁ - 3′-guanylic acid (inhibitor/product) complex. A possible scheme for the mechanism of action of RNase T₁ has been proposed on the basis of the arrangement of the catalytically important amino acid residues His40, Glu58, Arg77, and His92 around the guanosine ribose and the phosphate moiety in the RNase T₁ - GpC and RNase T₁ - G>p complexes. In this scheme, Glu58 serves as the general base group and His92 as the general acid group in the transphosphorylation step. His40 may be essential for stabilising the negatively charged phosphate moiety in the enzyme-transition state complex.     

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.     

Vibrational spectra and structure of M(CO2) and M2(CO2) molecules

Atomic Na, K and Cs were codeposited with CO₂ in excess of matrix gas at the temperature of 12 K. The IR spectra revealed the presence of ionic aggregates corresponding to the molecules M(CO)₂ and M₂(CO₂) (M=Na, K, Cs). Both molecular species have C_2v symmetry; M(CO₂) species have a planar ring structure while M₂(CO₂) have a W-shape structure. M₂(CO₂) molecules with C_s symmetry were also identified. The geometrical parameters of all the molecules were determined by ¹²C/¹³C and ¹⁶O/¹⁸O isotopic shifts. Raman spectra were also recorded and the results are reported in this study. The effect of photolysis on the structure of these molecules was examined. It was determined that photolysis promotes the formation of Na(CO₂) and transforms the M₂(CO₂) molecules with C_2v symmetry into C_s symmetry isomers.     

The Structure of Neplanocin C

Abstract

The molecular and crystal structure of neplanocin C(3), C₁₁H₁₃N₅O₄ M.W. = 279.26, has been determined by X-ray anlys?s. The space group is P2₁ with a=16.381(2), b=8.210(1), c=9.127(1) Å, β=105.31(1)° and z=4. The structure was solved by direct method, and least-squares refinement using 2093 reflections with |Fo|>3σ(F) led to the final R value of 0.0772. The sugar puckering of the two crystal-lographically independent molecules is C(2′)-exo-C(3′)-endo, and the torsion angles about the N(9)-C(1′) bond are 22.8(6) and 28.7(6)°, respectively (anti conformation).     

The dimensions and shapes of the furanose rings in nucleic acids

A survey was made of the geometry of furanose rings in beta-nucleotides and beta-nucleosides (as monomers related to nucleic acids) for which structures have been determined by X-ray crystallography. Mean values, and estimated standard deviations from them, were calculated for bond-lengths, bond-angles and conformation-angles. For parameters with values dependent on ring-puckering, separate calculations were made for each ring type. (The rings are puckered in one of three conformations: C-2- or C-3-endo or C-3-exo; C-2-exo has not been observed.) The results were used to compute standard furanose rings with C-2-endo, C-3-endo and C-3-exo conformations for use in nucleic acid molecular model-building. The survey also showed that the only other conformation-angle in nucleotides dependent on the furanose ring conformation corresponds to the relative orientation of the purine (or pyrimidine) base and the ring.     

Flexibility of the pyranose ring in α- and β-D-glucoses

Conformational energies of α- and β-D -glucopyranoses were computed by varying all the ring bond angles and torsional angles using semiempirical potential functions. Solvent accessibility calculations were also performed to obtain a measure of solvent interaction. The results indicate that the ⁴C₁ (D ) chair is the most favored conformation, both by potential energy and solvent accessibility criteria. The ⁴C₁ (D ) chair conformation is also found to be somewhat flexible, being able to accommodate variations up to 10° in the ring torsional angles without appreciable change in energy. Observed solid-state conformations of these sugars and their derivatives lie in the minimum-energy region, suggesting that the substituents and crystal field forces play a minor role in influencing the pyranose ring conformation. Theory also predicts the variations in the ring torsional angles, i.e., CCCC < CCCO < CCOC, in agreement with the experimental results. The boat and twist-boat conformations are found to be at least 5 kcal mol^?1 higher in energy compared to the ⁴C₁ (D ) chair, suggesting that these forms are unlikely to be present in a polysaccharide chain. The ¹C₄ (D ) chair has energy intermediate between that of the ⁴C₁ (D ) chair and that of the twist-boat conformation. The calculated energy barrier between ⁴C₁ (D ) and ¹C₄ (D ) conformations is high—about 11 kcal mol^?1.     

The Study of Possible A and B Conformations of Alternating DNA Using a New Program for Conformational Analysis of Duplexes (CONAN)

Abstract

A new program, CONAN has been designed for CONformational ANalysis of oligonucleotide duplexes with natural and modified bases. It allows to model both regular DNA fragments with different types of symmetry and irregular ones including bends, junctions, mismatched pairs and base lesions. Computations and minimization of the energy are performed in a space of internal structural variables chosen to build start structure easier and conveniently analyze the results obtained. These internal structural variables determine mutual base-base and base-sugar arrangement and sugar puckering. The analytical closure procedure is applied both to sugar rings and to backbone fragments between adjacent sugars. For more effective energy minimization, analytical gradient is calculated. The CONAN was applied to the search for low-energy conformations of poly(dA-dT)·poly(dA-dT) and poly(dG-dC)·poly(dG-dC) duplexes. Extended regions of low-energy A and B conformations are revealed and characterized. These regions contain structures with different relative values of helical twist, τ, for pur-pyr and pyr-pur steps, namely, conformations with τ(pur-pyr)>τ(pyr-pur) and with τ(pur-pyr)<τ(pyr-pur). Two types of sugar puckering were found for B-form low-energy conformations, the first type with all C2′-endo sugar residues and the second one—;with C2′-endo purines and O1′-endo pyrimidines. The calculated conformations are compared with X-ray diffraction data for crystals and fibers and NMR data for solution.     

The crystal structure of D-glucaro-1,4-lactone monohydrate

In the crystal structure of D-glucaro-1,4-lactone monohydrate, C₆H₈O₇·H₂O, the molecules have the E₃ lactone-ring conformation, with a small distortion of the ring to ₃T². The α-hydroxycarboxylic acid side-chain is axial, with the HO---C---C=O torsion angle within 6° of cis-planar. The orientation of the side-chain is such that the hydroxyl group lies over the lactone ring, which is the same conformation as is reported to preponderate in solution. Calculations of non-bonding repulsion energy show that this conformation corresponds to an energy minimum, although comparable minima can also be obtained with the ring in the alternative ³E conformation. The lactone and water molecules are hydrogen-bonded to form layers two molecules,wide, separated by Van der Waals interactions. One of the water hydrogen atoms is involved in a weak, bifurcated hydrogen-bond.     

Interactions of molecules with nucleic acids. IV. Binding energies and conformations of acridine and phenanthridine compounds in the two principal and in several unconstrained dimer-duplex intercalation sites

The binding positions and relative minimum binding energies are calculated for complexes of 9-aminoacridine, proflavine, N-methylphenanthridinium, and ethidium in theoretically determined intercalation sites in B-DNA (sites I and II) and in unconstrained dimer-duplex sites. The selection of site I in B-DNA by these compounds agrees with the theoretical interpretation of studies of unwinding angles in closed circular DNA in all cases but ethidium, which is predicted to select site II. The most stable binding positions of the acridines and ethidium in unconstrained dimer-duplex units agree with experimental results of intercalation complexes of dinucleoside monophosphate units. Base-pair specificity for Watson-Crick pairing is examined. The energy of an intercalation complex is partitioned into ΔE₂₃, the energy required to open base pairs BP₂ and BP₃ in B-DNA to a site, and ΔE_In, the energy change when a free molecular intercalates. ΔE₂₃ depends strongly on the base-pair sequence, whereas ΔE_In for the four molecules studied does not. The three most stable sequences contain (pyrimidine)p(purine) units, and this provides a rationale for the exclusive formation of crystals of intercalation complexes with these units. In spite of this selectivity, the distribution of G?C and A?T base pairs is equal for these three units and persists as the more unstable sequences are included. Therefore, specificity arises from the interaction between the base pairs and the 2′-deoxyribose 5′-monophosphate backbone for the opening of B-DNA to an intercalation site and not from the interaction between the chromophore and the DNA.     

Synthesis,FT-IR and 1H NMR studies of alkali and alkaline earth metal complexes with guanosine

The synthesis of complexes of Li(I), K(I), Mg(II), Ca(II) and Ba(II) with guanosine in basic non aqueous solutions is described. The complexes were of two types: (1) complexes having the general formula, M(Guo)_nX_m·YH₂O·ZC₂H₅OH, where M = Mg(II), Ca(II), Ba(II) and Li(I), n = 1,2,4, X = Cl^?, Br^?, NO₃^?, ClO₄^? and OH^?, m = 1,2, Y = 0?6 and X = 0?2, and (2) complexes with the general formula, M(GuoH-1)(OH)_n^?1·YH₂O, where M = K(I), Ca(Il) and Ba(II), GuoH-1 =Ionized guanosine at N₁, n = 1,2 and Y = 1?3. The complexes are characterized by their proton nuclear magnetic resonance (¹H NMR) and Fourier transform infrared (FT-IR) spectra. The FT-IR and ¹H NMR data of the non ionized nucleoside complexes suggest that the metal binding is through the N₇-site of guanine and that the anion (X) is hydrogen bonded to N₁H and NH₂ groups. In the N₁-ionized guanosine complexes the metal binding is via the O₆^? of guanine. All the complexes formed exhibited a transition of the sugar conformation from C₂′-endo/anti in the free nucleoside to C₃′-endo/anti in the metal complexes.