Molecular conformations of DNA and RNA subunits

Issued as Report of expenditures, Project no. G-41-64

Conformational stability in dinucleoside phosphate crystals. Semiempirical potential energy calculations for uridylyl-3'-5'-adenosine monophosphate (UpA) and guanylyl-3',5'-cytidine monophosphate (GpC)

Classical potential energy calculations were performed for the dinucleoside phosphates UpA and GpC. Two widely accessible low-energy regions of conformation space were found for the w', w pair. That of lowest energy contains conformations similar to helical RNA, with w' and w in the vicinity of 300° and 280°, respectively. All five experimental observations of crystalline GpC, two of ApU, and the helical fragment of ApApA fall in this range. The second lowest region has w' and w at about 20° and 80°, respectively, which is in the general region of one experimentally observed crystalline conformer of UpA, and the nonhelical region of ApApA. It is concluded that GpC and ApU, which were crystallized as either sodium or calcium salts, are shielded from each other in the crystal by the water of hydration and are therefore free to adopt their predicted in vacuo minimum energy helical conformations. By contrast, crystalline UpA had only 1/2 water per molecule, and was forced into higher energy conformations in order to maximize intermolecular hydrogen bonding

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

CONFORMATION OF THE C8 SUBSTITUTED GUANINE ADDUCT OF THE CARCINOGEN ACETYLAMINOFLUORENE - MODEL FOR A POSSIBLE Z-DNA MODIFIED STRUCTURE

The general problem of heavy-metal interactions with DNA bases has been investigated in this laboratory for several years. The methylmercury cation, a mutagenic agent, has been used to identify the potential sites of reaction for heavy metals. Results with 1-methylcytosine (mCyt) and unblocked cytosine (Cyt) are described in the present paper

The crystal and molecular structure of a calcium salt of guanylyl-3',5'-cytidine (GpC)

The calcium salt, Ca(C_19H_24N_8O_I2P)_2.18H_20, of guanylyl-3',5'-cytidine (GpC) has been refined to an R of 8·2 % for 2918 observed reflections (11% for 4237 reflections, including unobserved). The molecule crystallized in space group P2_1 with a=21·224, b=34·207, c=9·327 Å, β=90·527°, Z=4. The asymmetric unit contains four GpC, 36 waters and two Ca^2+ ions, for a total of 198 non-hydrogen atoms. The four GpC occur as two dimers related by a pseudo C-face-centering. Each dimer consists of two crystallographically independent GpC as Watson-Crick base-pairs, and possesses a pseudo twofold axis broken by a Ca^2+ ion and associated solvent. The structure was solved by an unusual series of steps including semi-empirical potential-energy methods, packing analysis, rigid-body refinement, least-squares and difference Fourier techniques, and direct-methods tangent-formula phase refinement. The four GpC have conformational angles in the range of helical RNA, but are not identical. The different crystallographic environments perturb the GpC from exact symmetry and demonstrate the range of the basic helical conformations. All eight bases are anti, sugars are all C(3’) endo, the C(4')-C(5') bond rotations are gauche-gauche, and the ω', ω angle pair about the O-P bonds is gauche—gauche-

Structure of guanylyl-3′,5′-cytidine monophosphate. II. Description of the molecular and crystal structure of the calcium derivative in space group P2₁

The structural features of calcium guanosine-3′,5′-cytidine monophosphate (GpC) have been elucidated by X-ray diffraction analysis. The molecule was crystallized in space group P2₁ with cell constants of a = 21.224 Å, b = 34.207 Å, c = 9.327 Å, and β = 90.527°, Z = 8. The hydration of the crystal is 21% by weight with 72 water molecules in the unit cell. The four GpC molecules in the asymmetric unit occur as two Watson-Crick hydrogen-bonded dimers related by a pseudo-C face centering. Each dimer consists of two independent GpC molecules whose bases are hydrogen bonded to each other in the traditional Watson-Crick fashion. Each dimer possesses a pseudo twofold axis broken by a calcium ion and associated solvent. The four molecules are conformationally similar to helical RNA, but are not identical to it or to each other. Instead, values of conformational angles reflect the intrinsic flexibility of the molecule within the range of basic helical conformations. All eight bases are anti, sugars are all C3′-endo, and the C4′-C5′ bond rotations are gauche-gauche. The R factor is 12.6% for 2918 observed reflections at 1.2-Å resolution

Conformation of Guanosine Cytidine 3',5'-Monophosphate (GpC)

A brief communication of preliminary results of solution of dinucleoside phosphate GpC

Structure of guanosine-3′,5′-cytidine monophosphate. I. Semi-empirical potential energy calculations and model-building

The conformation and packing scheme for guanosine-3’,5’-cytidine monophosphate, GpC, were computed by minimizing the classical potential energy. The lowest energy conformation of the isolated molecule had dihedral angles in the range of helical RNA’s, and the sugar pucker was C3‘ endo. This was used as the starting conformation in a packing search over orientation space, the dihedral angles being flexible in this step also. The packing search was restricted by constraints from our x-ray data, namely, (1) the dimensions of the monoclinic unit cell and its pseudo-C2 symmetry (the real space group is P21), (2) t,he location of the phosphorous atom, and (3) the orientation of the bases. In addition, a geometric function was devised to impose Watson-Crick base pairing. Thus, a trial structure could be sought without explicit inclusion of intermolecular potentials. An interactive computer graphics system was used for visualizing the calculated structures. The packing searches yielded two lowest energy schemes in which the molecules had the same conformation (similar to double-helical RNA) but different orientations within the unit cell. One of these was refined by standard x-ray methods to a discrepancy index of 14.4% in the C2 pseudocell. This served as the starting structure for the subsequent refinement in the real P21 cell

Classical potential energy calculations for ApA, CpC, GpG, and UpU. The influence of the bases on RNA subunit conformations

Classical potential energy calculations have been made for the ribodinucleoside monophosphates ApA, CpC, GpG, and UpU. Van der Waal's, electrostatic, and torsional contributions to the energy were calculated, and the energy was minimized with the seven backbone conformational angles as simultaneously variable parameters. At the global minimum, ApA and CpC have conformations like double helical RNA: the angles ω′ and ω are g−g−, the sugar pucker is C3′-endo, and the bases are anti. GpG and UpU, on the other hand, have the ω′,ω angle pair g−t at the global minimum, and for GpG the bases are syn. Energy contour maps for ω′ and ω show two broad, low energy regions for ApA, CpC, and UpU: one is g−g−, and the second encompasses g−t and g+g+ within a single low energy contour. The two regions are connected by a path at 10–13 kcal./mole. For GpG, with bases syn, however, only a small low-energy region at g−t is found. The helical ‘A’ RNA conformation is 8.5 kcal/mole higher for this molecule. Thus, the base composition is shown to influence the conformations adopted by dinucleoside phosphates. Comparison of calculations with experimental data, where available, show good agreement

DNA Backbone Conformation in Cis-Syn Pyrimidine[ ]Pyrimidine Cyclobutane Dimers

A theoretical calculation involving minimization of energy functions was made to determine the conformation of a deoxydinucleoside monophosphate pyrimidine[ ]pyrimidine cis-syn cyclobutane dimer. Such single-stranded moieties are useful models for the in uiuo situation because single strands are more easily damaged, and the damage inhibits the normal function of single-stranded replicating DNA. The calculated minimum-energy conformer was incorporated in a mode l of B-DNA to assess the influence of this covalent lesion on the normal form of DNA