Molecular structure of a DNA decamber containing an anticancer nucleoside arabinosylcytosine: conformational perturbation by arabinosylcytosine in B-DNA

Arabinosylcytosine (araC) is an important anticancer drug that has been shown to be misincorporated into DNA double helix. The incorporation of araC into DNA may have significant conformational consequences that could affect the function of DNA. In this paper, we present the high-resolution 3D structure of an araC-containing decamer d[CCAGGC(araC)TGG], as determined by X-ray diffraction analysis, and assess the possible DNA structural perturbation induced by araC. The modified decamer was crystallized in the monoclinic C2 (a = 31.97 A, b = 25.56 A, c = 34.62 A and beta = 114.50 degrees) space group, the same as that from d(CCAGGCCTGG) [Heinemann, U., & Alings, C. (1989) J. Mol. Biol. 210, 369]. The structure of the araC-containing decamer was solved by the molecular replacement method and refined by the constrained least-squares refinement procedure to obtain a final R factor of 0.187 using 2349 [greater than 2.0 sigma(F)] observed reflections to a resolution of 1.6 A. The overall conformation resembles that of the canonical decamer DNA structure, but with significant differences in regions close to the araC site. The O2' hydroxyl groups of the araC residues lie in the major groove of the helix, and they are in close contact with the C5 methyl and C6 H6 atoms of the thymine on the 3'-side. This creates a higher buckle in the araC7-G14 base pair (14 degrees), as compared to that found in the canonical decamer (9 degrees). This may slightly destabilize B-DNA. No direct intramolecular hydrogen bond is formed, in contrast to the situation when araC is incorporated into Z-DNA.(ABSTRACT TRUNCATED AT 250 WORDS)     

The structure of B-helical C-G-A-T-C-G-A-T-C-G and comparison with C-C-A-A-C-G-T-T-G-G. The effect of base pair reversals

The crystal structure of the DNA decamer C-G-A-T-C-G-A-T-C-G has been solved to a resolution of 1.5 A, with a final R-factor of 16.1% for 5,107 two-sigma reflections. Crystals are orthorhombic space group P2(1)2(1)2(1), with cell dimensions a = 38.93 A, b = 39.63 A, c = 33.30 A, and 10 base pairs/asymmetric unit. The final structure contains 404 DNA atoms, 142 water molecules treated as oxygen atoms, and two Mg(H2O)6(2+) complexes. Decamers stack atop one another to simulate continuous helical columns through the crystal, as with three previously solved monoclinic decamers, but the lateral contacts between columns are quite different in the orthorhombic and monoclinic cells. Narrow and wide regions of the minor groove exhibit a single spine or two ribbons of hydration, respectively, and the minor groove is widest when BII phosphate conformations are opposed diagonally across the groove. Phosphate conformation, in turn, appears to have a base sequence dependence. Twist, rise, cup, and roll are linked as has been observed in the three monoclinic decamers and can be characterized by high or low twist profiles. In all five known decamer crystal structures and eight representative dodecamers, a high twist profile is observed with G-C and G-A steps whereas all other R-R steps are low twist profiles (R = purine). A-T and A-C steps are intermediate in character whereas C-A and C-G exhibit behavior that is strongly influenced by the profiles of the preceding and following steps. When sufficient data are in hand, sequence/structure relationships for all helix parameters probably should be considered in a 4-base pair context. At this stage of limited information the problem is compounded because there are 136 unique 4-base steps x-A-B-y in a double helix as compared with only 10 2-base steps A-B.     

Structure of a B-DNA decamer with a central T-A step: C-G-A-T-T-A-A-T-C-G.

The X-ray crystal structure analysis of the decamer C-G-A-T-T-A-A-T-C-G has been carried out to a resolution of 1.5 A. The crystals are space group P2(1)2(1)2(1), cell dimensions a = 38.60 A, b = 39.10 A, c = 33.07 A. The structure was solved by molecular replacement and refined with X-PLOR and NUCLSQ. The final R factor for a model with 404 DNA atoms, 108 water molecules and one magnesium hexahydrate cation is 15.7%. The double helix is essentially isostructural with C-G-A-T-C-G-A-T-C-G, with closely similar local helix parameters. The structure of the T-T-A-A center differs from that found in C-G-C-G-T-T-A-A-C-G-C-G in that the minor groove in our decamer is wide at the central T-A step rather than narrow, and the twist angle of the T-A step is small (31.1 degrees) rather than large. Whereas the tetrad model provides a convenient framework for discussing local DNA helix structure, it cannot be the entire story. The articulated helix model of DNA structure proposes that certain sequence regions of DNA show preferential twisting or bending properties, whereas other regions are less capable of deformation, in a manner that may be useful in sequence recognition by drugs and protein. Further crystal structure analyses should help to delineate the precise nature of sequence-dependent articulation in the DNA double helix.     

Crystal structure of chartreusin derivative A132

The crystal structure of chartreusin derivative A132 (benzilidene chartreusin) has been determined by single-crystal X-ray diffraction. The space group is C2 with unit cell dimensions, a=18.482(4), b=8.749(3), c=43.906(2) A, beta=94.87(2) degrees, and the structure was refined to R-factors of 0.2365 (6585 all unique reflections) and 0.087 (2914 reflections with F(o)>4 sigma(F(o))) by a full-matrix least-squares method. There are two molecules in an asymmetric unit. Both molecules have similar structures, which are favorable to bind with DNA in the minor groove. A modeling study of the A132-DNA complex based on the X-ray structures suggests that the sugar moiety of A132 may play an important role in recognizing the sequence of DNA base pairs.     

Conformation and hydrogen bonding of N-formylmethionyl peptides. II. Crystal and molecular structure of N-formyl-L-methionyl-L-phenylalanine

Crystals of N-formyl-L-methionyl-L-phenylalanine (C15H20N2O4S), grown from aqueous methanol solution are orthorhombic, space group, P2(1)2(1)2(1), with cell parameters at 294K of a = 4.900(2), b = 17.947(4), c = 18.726(4)A, V = 1646.8A3, M.W. = 324.4, Z = 4 and Dm = 1.308 g/cc, and as expected, all nearly identical to that of N-f-D-Met-D-Phe studied by Jeffs, Heald, Chodosh & Eggleston (Int. J. Peptide Protein Res. 24, 442-446, 1984). The crystal structure was solved and refined using CAD-4 data (1095 reflections greater than or equal to 3 sigma) to a final R value of 0.042. Molecules related by the alpha-translation form a parallel beta-sheet rather than anti-parallel sheet as stated in the earlier study of Jeffs et al. The formation of the parallel rather than the anti-parallel beta-sheet structure, the use of the C-H ...O hydrogen bonds to stabilize the beta-sheet and the very short O-H ...O hydrogen bond between the carboxyl OH and the N-acyl oxygen atom emerge as the main structural features of the chemotactic N-formyl methionyl peptides.     

Crystallization and preliminary X-ray diffraction studies of a deglycosylated glucose oxidase from Penicillium amagasakiense.

The dimeric glucose oxidase from Penicillium amagasakiense was deglycosylated, purified and crystallized as a complex with its coenzyme FAD. Deglycosylation and purification to isoelectric homogeneity were shown to be an important prerequisite step to obtain crystals suitable for X-ray investigations. Crystals of the deglycosylated enzyme were reproducibly grown using ammonium sulfate as precipitant at pH 7.4 to 7.5. Crystals diffract to at least 2.0 A resolution and belong to the orthorhombic space group P2(1)2(1)2(1), with refined lattice constants of a = 59.3 A, b = 136.3 A and c = 156.7 A. Assuming two monomers (approximately 135 kDa) per asymmetric unit the Vm value is 2.3 A3/Da.     

Crystallization of complexes of EcoRV endonuclease with cognate and non-cognate DNA fragments

Complexes of the type II restriction endonuclease EcoRV with a variety of short, selfcomplementary deoxyoligonucleotides have been crystallized. The best crystals diffract to about 2.7 A resolution and consist of 1:1 complexes between endonuclease dimers and duplexes of the cognate decamer GGGATATCCC containing the hexameric RV recognition sequence GATATC. Crystals with the non-cognate DNA octamer duplexes CGAGCTCG and CGAATTCG diffract to 3.0 and 3.5 A resolution, respectively, and contain two DNA duplexes per enzyme dimer.     

A novel end-to-end binding of two netropsins to the DNA decamers d(CCCCCIIIII)2, d(CCCBr5CCIIIII)2and d(CBr5CCCCIIIII)2.

Netropsin is bound to the DNA decamer d(CCCCCIIIII)2, the C-4 bromo derivative d(CCCBr5CCIIIII)2and the C-2 bromo derivative d(CBr5CCCCIIIII)2in a novel 2:1 mode. Complexes of the native decamer and the C-4 bromo derivative are isomorphous, space group P1, unit cell dimensions a = 32.56 A (32.66), b = 32.59 A (32.77), c = 37.64 A (37.71), alpha = 86.30 degrees (86.01 degrees), beta = 84.50 degrees (84.37 degrees), gamma = 68.58 degrees (68.90 degrees) with two independent molecules (A and B) in the asymmetric unit (values in parentheses are for the derivative). The C-2 bromo derivative is hexagonal P61, unit cell dimensions a = b = 32.13 A, c = 143.92, gamma = 120 degrees with one molecule in the asymmetric unit. The structures were solved by the molecular replacement method. The novelty of the structures is that there are two netropsins bound end-to-end in the minor groove of each B-DNA decamer which has nearly a complete turn. The netropsins are held by hydrogen bonding interactions to the base atoms and by sandwiching van der Waal's interactions from the sugar-phosphate backbones of the double helix similar to every other drug.DNA complex. Each netropsin molecule spans approximately 5 bp. The netropsins refined with their guanidinium heads facing each other at the center, although an orientational disorder for the netropsins cannot be excluded. The amidinium ends stretch out toward the junctions and bind to the adjacent duplexes in the columns of stacked symmetry-related complexes. Both cationic ends of netropsin are bridged by water molecules in one of the independent molecules (molecule A) of the triclinic structures and also the hexagonal structure to form pseudo-continuous drug.decamer helices.     

Crystal structure of L-2-oxothiazolidine-4-carboxylic acid

Crystals of the title compound, L-2-oxothiazolidine-4-carboxylic acid, OTC (C4H5NO3S), grown from an aqueous solution are orthorhombic, space group P2(1)2(1)2(1) with the following cell parameters at 22 +/- 3 degrees: a = 5.381(1), b = 5.961(1), c = 17.929(3)A, V = 575.1A(3), Mr = 146.2, Dc = 1.688 g.cm-3, mu = 43.9 cm-1 and Z = 4. The crystal structure was solved by the application of direct methods and refined to an R value of 0.032 for 596 reflections with I greater than 3 sigma(I). The thiazolidine ring adopts a "twist" conformation. This structure contains a short (2.619(3)A) intermolecular hydrogen bond between the carboxyl OH and the oxygen of the 2-oxo moiety, a feature common to most acyl amino acids and acyl peptides.     

Crystallization and preliminary X-ray studies of the pectate lyase from Bacillus subtilis.

The pectate lyase (EC 4.2.2.9) from Bacillus subtilis has been crystallized. Crystals of form 1, grown by the hanging drop method using polyethylene glycol as precipitant, diffract to at least 2.4 A resolution. They belong to the spacegroup P2(1) with a = 132.9 A, b = 41.2 A, c = 156.8 A and beta = 114.9 degrees with probably four molecules in the asymmetric unit. A second crystal form grown from 2-methyl-2,4-pentandiol also belongs to the spacegroup P2(1) with a = 55.0 A, b = 88.1 A, c = 50.2 A and beta = 109.0 degrees. These crystals diffract to at least 2.0 A and have one molecule in the asymmetric unit. Both crystal forms are suitable for the determination of high-resolution structures.     

RNA-protein interactions in some small plant viruses

The structure of the three quasi-equivalent protein subunits A, B and C of the spherical, T = 3 southern bean mosaic virus (SBMV) have been carefully built in accordance with a refined electron density map of the complete virus. The lower electron density in the RNA portion of the map could not be explicitly interpreted in terms of a preferred RNA structure on which some icosahedral symmetry might have been imposed. However, the extremely basic nature of the interior surface of the coat protein must be associated with the binding and organization of the RNA. Comparison with the small spherical, T = 1 satellite tobacco necrosis virus (STNV; Liljas et al., J. Mol. Biol. 159, 93-108, 1982) and the T = 1 aggregate of alfalfa mosaic virus (AMV) protein (Fukuyama et al., J. Mol. Biol. 150, 33-41, 1981) showed similar results. The pattern of basic residues on the SBMV coat protein surface facing the RNA is able to dock a 9 base pair double-helical A-RNA structure with surprising accuracy. The basic residues are each associated with a different phosphate and the protein can make interactions with five bases in the minor groove. This may be one of a small number of ways in which the RNA interacts with SBMV coat protein. The self-assembly of SBMV has been studied in relation to the presence of the 63 basic amino-terminal coat protein sequence, pH, Ca2+ and Mg2+ ions and RNA. These results have led to a two-state model where the "relaxed" dimers initially self-assemble into 10-mer caps which nucleate the assembly of T = 1 or T = 3 capsids depending on the charge state of the carboxyl group clusters in the subunit contact region. The two-state condition of dimers in a viral coat protein extends the range of structures originally envisaged by Caspar and Klug (Cold Spring Harbor Symp. Quant. Biol. 27, 1-24, 1962).     

Conformational perturbation of the anticancer nucleotide arabinosylcytosine on Z-DNA: molecular structure of (araC-dG)3 at 1.3 A resolution.

The left-handed Z-DNA structure of an araC-containing (where araC stands for arabinosylcytosine) hexamer, (araC-dG)3, has been solved by x-ray diffraction analysis at 1.3 A resolution. This hexamer was crystallized in the hexagonal P6(5)22 (a = b = 17.96 A, c = 43.22 A) space group in which the hexamers have statistically disordered packing arrangement along the 6(5) screw axis, yet the crystals diffract x-rays to high resolution. Its structure has been refined by the constrained least square refinement to a final R factor of 0.287 using 737 [> 3.0 sigma(F)] observed reflections. The asymmetric unit of the unit cell contains only a dinucleotide, 5'-p (araC)p(dG). The overall conformation resembles that of the canonical Z-DNA, but with some differences in details. The O2' hydroxyl groups of the araC residues form intramolecular hydrogen bonds with N2 of the 5'-guanine residues. In the deep groove of Z-DNA, these hydroxy groups replace the bridging water molecules that stabilize the guanine in the syn conformation. The results reinforce the earlier observation made by the structural analysis of another hexamer, d(CG[araC]GCG), with a mono-substitution of araC [M.-K. Teng, Y.-C. Liaw, G. A. van der Marel, J. H. van Boom, and A. H.-J. Wang (1989) Biochemistry, vol. 28, pp. 4923-4928]. These two structures show that araC residue can be incorporated readily into the Z structure and probably facilitates the B to Z transition, as supported by uv absorption spectroscopic studies in a number of araC-containing oligonucleotides. The potential biological roles of the araC-modified Z-DNA are discussed.     

Structure of Paramecium tetraurelia calmodulin at 1.8 A resolution.

The crystal structure of calmodulin (CaM; M(r) 16,700, 148 residues) from the ciliated protozoan Paramecium tetraurelia (PCaM) has been determined and refined using 1.8 A resolution area detector data. The crystals are triclinic, space group P1, a = 29.66, b = 53.79, c = 25.49 A, alpha = 92.84, beta = 97.02, and gamma = 88.54 degrees with one molecule in the unit cell. Crystals of the mammalian CaM (MCaM; Babu et al., 1988) and Drosophila CaM (DCaM; Taylor et al., 1991) also belong to the same space group with very similar cell dimensions. All three CaMs have 148 residues, but there are 17 sequence changes between PCaM and MCaM and 16 changes between PCaM and DCaM. The initial difference in the molecular orientation between the PCaM and MCaM crystals was approximately 7 degrees as determined by the rotation function. The reoriented Paramecium model was extensively refitted using omit maps and refined using XPLOR. The R-value for 11,458 reflections with F > 3 sigma is 0.21, and the model consists of protein atoms for residues 4-147, 4 calcium ions, and 71 solvent molecules. The root mean square (rms) deviations in the bond lengths and bond angles in the model from ideal values are 0.016 A and 3 degrees, respectively. The molecular orientation of the final PCaM model differs from MCaM by only 1.7 degrees. The overall Paramecium CaM structure is very similar to the other calmodulin structures with a seven-turn long central helix connecting the two terminal domains, each containing two Ca-binding EF-hand motifs. The rms deviation in the backbone N, Ca, C, and O atoms between PCaM and MCaM is 0.52 A and between PCaM and DCaM is 0.85 A. The long central helix regions differ, where the B-factors are also high, particularly in PCaM and MCaM. Unlike the MCaM structure, with one kink at D80 in the middle of the linker region, and the DCaM structure, with two kinks at K75 and I85, in our PCaM structure there are no kinks in the helix; the distortion appears to be more gradually distributed over the entire helical region, which is bent with an apparent radius of curvature of 74.5(2) A. The different distortions in the central helical region probably arise from its inherent mobility.     

Crystallographic study of one turn of G/C-rich B-DNA

The DNA decamer d(CCAGGCCTGG) has been studied by X-ray crystallography. At a nominal resolution of 1.6 A, the structure was refined to R = 16.9% using stereochemical restraints. The oligodeoxyribonucleotide forms a straight B-DNA double helix with crystallographic dyad symmetry and ten base-pairs per turn. In the crystal lattice, DNA fragments stack end-to-end along the c-axis to form continuous double helices. The overall helical structure and, notably, the groove dimensions of the decamer are more similar to standard, fiber diffraction-determined B-DNA than A-tract DNA. A unique stacking geometry is observed at the CA/TG base-pair step, where an increased rotation about the helix axis and a sliding motion of the base-pairs along their long axes leads to a superposition of the base rings with neighboring carbonyl and amino functions. Three-center (bifurcated) hydrogen bonds are possible at the CC/GG base-pair steps of the decamer. In their common sequence elements, d(CCAGGCCTGG) and the related G.A mismatch decamer d(CCAAGATTGG) show very similar three-dimensional structures, except that d(CCAGGCCTGG) appears to have a less regularly hydrated minor groove. The paucity of minor groove hydration in the center of the decamer may be a general feature of G/C-rich DNA and explain its relative instability in the B-form of DNA.     

Direct determination of crystallographic phases for diffraction data from lipid bilayers. I. Reliability and phase refinement.

Direct analysis of lipid lamellar packing based on the probabilistic estimate of sigma 1- and sigma 2-triplet phase invariants is evaluated here for a large variety of bilayer structures than examined in an original study of this problem (Dorset, D.L., 1990. Biophys. J. 58:1077-1087). Using x-ray crystal structures of five phospholipids, three glycerides and two cerebrosides, lamellar diffraction data were generated at the approximately 3 A resolution often found experimentally from oriented multilayers. For structures where no significant density occurs at the unit cell origin, the ab initio phase determination is successful for six of the ten structures. A seventh structure can be solved if a limited set of sigma 2-triples are used to determine the initial phase set based on the hierarchy of the A2 values. Bilayers, e.g., with solvent at the origin, can be analyzed if a modified criterion for accepting phase estimates for sigma 1-triples is used, as suggested by the distribution of normalized structure factors and the number of probable single-valued phase domains. In all cases, partial phase determinations can be refined effectively by density modification ("flattening") of the hydrocarbon region in real space. A figure of merit suggested by Luzzati et al. (Luzzati, V., A. Tardieu, and D. Taupin. 1972. J. Mol. Biol. 64:269-286) used to evaluate the success of such refinement can be supplemented by an evaluation of density smoothness, which can also detect the presence of near structure homomorphs not identified by the former test for density flatness.     

Crystallization of and preliminary X-ray data for the negative regulator (AmiC) of the amidase operon of Pseudomonas aeruginosa.

The negative regulator (AmiC) of the amidase operon of Pseudomonas aeruginosa has been purified from an over-expressing clone and crystalized. Crystals of diffraction quality were obtained from polyethylene glycol 4000 and ammonium sulphate. AmiC crystallizes in P4(2)2(1)2 (a = 104.4 A, c = 66.6 A) with one subunit in the asymmetric unit. Crystals diffract beyond 2.8 A.     

Structure and conformation of linear peptides. VIII. Structure of t-Boc-glycyl-L-phenylalanine

The crystal structure of t-Boc-glycyl-L-phenylalanine (C14H22N2O5, molecular weight = 298) has been determined. Crystals are monoclinic, space group P2(1), with a = 7.599(1) A, b = 9.576(2), c = 12.841(2), beta = 97.21(1) degrees, Z = 2, Dm = 1.149, Dc = 1.168 g X cm-3. Trial structure was obtained by direct methods and refined to a final R-index of 0.064 for 1465 reflections with I greater than 1 sigma. The peptide unit is trans planar and is nearly perpendicular to the plane containing the urethane moiety. The plane of the carboxyl group makes a dihedral angle of 16.0 degrees with the peptide unit. The backbone torsion angles are omega 0 = -176.9 degrees, phi 1 = -88.0 degrees, psi 1 = -14.5 degrees, omega 1 = 176.4 degrees, phi 2 = -164.7 degrees and psi 2 = 170.3 degrees. The phenylalanine side chain conformation is represented by the torsion angles chi 1 = 52.0 degrees, chi 2 = 85.8 degrees.     

Crystallization of and preliminary X-ray data for the mouse major urinary protein and rat alpha-2u globulin.

Crystals of the mouse major urinary protein (MUP) and rat alpha-2u globulin (AMG) have been grown from solutions of polyethylene glycol 3350 and CdCl2, respectively. The crystals differ both in their morphologies and space groups but have very similar unit cell sizes. AMG crystallized in P2(1) (a = 56.6 A, b = 103.8 A, c = 62.7 A, beta = 95.1 degrees) with four subunits/asymmetric unit, while MUP gave crystals in P4(1)2(1)2 or P4(3)2(1)2 (a = 57.3 A, c = 109.9 A) with one subunit/asymmetric unit. Both crystal forms diffract beyond 2.8 A resolution.     

Crystal structure and conformation of L-pyroglutamyl-L-alanine

Crystals of the dipeptide, pyroglutamyl-alanine (C8H12N2O4) grown from aqueous methanol are monoclinic, space group P2(1) with the following cell parameters: a = 4.863(2), b = 16.069(1), c = 6.534(2)A and beta = 109.9(2) degrees, V = 480.0A3, Mr = 200.2, Dc = 1.385 g cm-3, and Z = 2. The crystal structure was solved by the application of direct methods and refined to an R value of 0.044 for 699 reflections with I greater than 2 sigma. The amide of the pyroglutamyl side chain is cis, omega 1 = 2.6(7) degrees; the peptide unit is trans and appreciably non-planar (omega 2 = 167.4(5) degrees). The backbone torsional angles are: psi 1 = 166.1(5), phi 2 = -90.3(6), and psi 2 = -22.4(6) degrees. This structure contains a short (2.551(5)A) intermolecular hydrogen bond between the carboxyl OH and the N-acyl oxygen, a feature common to most acyl amino acids and acyl peptides.