Base only binding of spermine in the deep groove of the A-DNA octamer d(GTGTACAC)

The crystal structure of a complex of spermine with the DNA octamer d(GTGTACAC) has been determined at 2.0-A resolution. The alternating sequence adopts an A-DNA conformation with a novel purine-purine extra-Watson-Crick hydrogen bond involving the central guanine G3 (G11) and adenine A13 (A5) in the deep groove. The oligocation spermine binds in the floor of the deep groove by interacting with the bases and assumes an S-shape. Its dyad is coincident with that of the DNA, reminiscent of repressor binding to B-DNA. The terminal and central ammonium groups of the top half of spermine form hydrogen-bonding interactions to the 5'-bases, GTG, of one strand; then the spermine winds across the groove to interact with the corresponding set of bases on the other strand. The methylene groups of spermine form a hydrophobic cluster with the methyl groups of the thymines and the O6 atoms of the guanines of the TGT sequences on either side of the dyad. The observed mode of binding of spermine to A-DNA can serve as a model for deep groove binding in RNA and DNA-RNA hybrids that show a propensity also for the A-conformation. It will be of interest to see if base binding of spermine to DNA is involved in the regulation of gene expression, since spermine and other oligocations are ubiquitous in cells and their concentration is coupled to stages in cell cycle.     

Sequence-dependent conformation of an A-DNA double helix. The crystal structure of the octamer d(G-G-T-A-T-A-C-C)

The crystal structures of the synthetic self-complementary octamer d(G-G-T-A-T-A-C-C) and its 5-bromouracil-containing analogue have been refined to R values of 20% and 14% at resolutions of 1.8 and 2.25 A, respectively. The molecules adopt and A-DNA type double-helical conformation, which is minimally affected by crystal forces. A detailed analysis of the structure shows a considerable influence of the nucleotide sequence on the base-pair stacking patterns. In particular, the electrostatic stacking interactions between adjacent guanine and thymine bases produce symmetric bending of the double helix and a major-groove widening. The sugar-phosphate backbone appears to be only slightly affected by the base sequence. The local variations in the base-pair orientation are brought about by correlated adjustments in the backbone torsion angles and the glycosidic orientation. Sequence-dependent conformational variations of the type observed here may contribute to the specificity of certain protein-DNA interactions.     

Effect of crystal packing environment on conformation of the DNA duplex. Molecular structure of the A-DNA octamer d(G-T-G-T-A-C-A-C) in two crystal forms

The structure of the octamer d(G-T-G-T-A-C-A-C) was determined in two different crystal forms, tetragonal P4(3)2(1)2 and hexagonal P6(1)22. Although in both forms the octamer adopts an A-DNA structure, there are significant conformational differences between them. In particular, the P-05' and the C5'-C4' bonds of the middle adenine (A5) residue exhibit a distorted trans-trans conformation in the tetragonal form, while they adopt the standard gauche-, gauche+ conformation in the hexagonal form. These differences can be correlated with certain features of the crystal packing interactions in the two forms. Furthermore, a comparison of the structures of various A-DNA octamers reveals that the A-form can be divided into two subclasses such that the hexagonal structures have helical and base pair parameters that fall closer to fiber A-DNA values, while in the tetragonal structures these parameters deviate more from fiber A-DNA. These results indicate that environment plays a major role in determining DNA conformation.     

Crystal and molecular structure of the alternating dodecamer d(GCGTACGTACGC) in the A-DNA form: comparison with the isomorphous non-alternating dodecamer d(CCGTACGTACGG).

The crystal structure of the alternating dodecamer d(GCGTACGTACGC) (5'-GC) has been determined to a resolution of 2.55A using oscillation film data. The crystals belong to space group P6(1) 22, a = b = 46.2A, c = 71.5A with one strand in the asymmetric unit, and are isomorphous with a previously described non-alternating dodecamer, d(CCGTACGTACGG) (5'-CC). Refinement by X-PLOR/NUCLSQ gave a final R factor of 14.2% for 1089 observations. The molecule adopts the A-DNA form. The interchange of the terminal base pairs in the two dodecamers results in differences in the intermolecular contacts and may account for the differences in the bending. This dodecamer shows an axial deflection of 30 degrees, in the direction of the major groove compared to 20 degrees in 5'-CC and may be a consequence of additional contacts generated in 5'-GC by the interchange of end base pairs. The high helical axis deflection appreciably influences the local helical parameters. The molecule exhibits relatively high inclination angles, and has a narrow major groove. The helical parameters when described relative to the dyad-related hexamer halves of the molecule give more reasonable values. The crystal packing, local helical parameters, torsion angles, and hydration are described and also compared with the non-alternating 5'-CC dodecamer.     

Molecular structure of an A-DNA decamer d(ACCGGCCGGT)

The molecular structure of the DNA decamer d(ACCGGCCGGT) has been solved and refined by single-crystal X-ray-diffraction analysis at 0.20 nm to a final R-factor of 18.0%. The decamer crystallizes as an A-DNA double helical fragment with unit-cell dimensions of a = b = 3.923 nm and c = 7.80 nm in the space group P6(1)22. The overall conformation of this A-DNA decamer is very similar to that of the fiber model for A-DNA which has a large average base-pair tilt and hence a wide and shallow minor groove. This structure is in contrast to that of several A-DNA octamers in which the molecules all have low base-pair-tilt angles (8-12 degrees) resulting in an appearance intermediate between B-DNA and A-DNA. The average helical parameters of this decamer are typical of A-DNA with 10.9 base pairs/turn of helix, an average helical twist angle of 33.1 degrees, and a base-pair-tilt angle of 18.2 degrees. However, the CpG step in this molecule has a low local-twist angle of 24.5 degrees, similar to that seen in other A-DNA oligomers, and therefore appears to be an intrinsic stacking pattern for this step. The molecules pack in the crystal using a recurring binding motif, namely, the terminal base pair of one helix abuts the surface of the shallow minor groove of another helix. In addition, the GC base pairs have large propeller-twist angles, unlike those found most other A-DNA structures.     

Crystal and molecular structure of the A-DNA dodecamer d(CCGTACGTACGG). Choice of fragment helical axis.

The crystal structure of the dodecamer d(CCGTACGTACGG) has been determined at 2.5 A resolution. The crystals grow in the hexagonal space group P6(1)22, a = b = 46.2 A, c = 71.5 A with one strand as the asymmetric unit. Diffraction data were collected by the oscillation film method yielding 1664 unique reflections with an Rmerge of 0.04. The structure was solved by real-space rotational translational searches with idealized helical models of A, B and Z-DNA. The best agreement was given by an A-DNA model with its dyad axis along the diagonal crystallographic dyad axis, with an R-factor 0.43 and correlation coefficient of 0.59 for data between 10 and 5 A. Iterative map fitting and restrained least-squares refinement and addition of 40 solvent molecules brought the R-factor to 0.15 and the correlation coefficient to 0.97 for all data between 8.0 and 2.5 A. The stereochemistry of the atomic model is good, with a root-mean-square deviation in bond distances of 0.006 A. This is the first example of an A-DNA containing a full helical turn. The dodecamer displays a novel packing motif. In addition to the characteristic contacts between the terminal base-pairs and the minor grooves of symmetry-related molecules, there are also minor groove to minor groove interactions not previously observed. The packing leaves an approximately 25 A diameter solvent channel around the origin, along the c-axis. The presence of a prominent 3.4 A meridional reflection and other diffuse features in the diffraction pattern provided evidence for the presence of disordered B-DNA along the c-axis, which can be accommodated in these solvent channels. The molecular conformation of the dodecamer also displays novel features. The dyad-related halves of the molecule are bent at an angle of 20 degrees, and the helical parameters are affected by this bend. Unlike the shorter A-DNA octamers, the dimensions of the major groove can be directly measured. Novel correlations between local helical parameters and global conformational features are presented. Most of the solvent molecules are associated with the major groove and the sugar-phosphate backbone.     

High-resolution A-DNA crystal structures of d(AGGGGCCCCT). An A-DNA model of poly(dG) x poly(dC).

A-DNA conformation is favored by guanine-rich sequences, such as (dG)n x (dC)n, or under low-humidity conditions. Earlier A-DNA crystal structures revealed some conformational variations which may be the result of sequence-dependent effects and/or crystal packing forces. Here we report the high-resolution crystal structure of d(AGGGGCCCCT) in two crystal forms (either in the P212121 or the P6122 space group) to gain insights into the conformation and dynamics of the (dG)n x (dC)n sequence. The P212121 form has been analyzed using data to 1.1 A resolution by the anisotropic temperature factor refinement procedure of the SHELX97 program. Such analysis affords us with the detailed geometric, conformational and motional property of an A-DNA structure. The backbone torsional angles fall in a narrow range, except for the alpha/gamma angles which have two distinct combinations (gauche-/gauche+ or trans/trans). An A-DNA model of poly(dG) x poly(dC) has been constructed using the conformational parameters derived from the crystal structure of the P212121 form. In the crystal structure of the P6122 space group, the central eight base pairs of the decamer adopt A-DNA conformation with the two terminal nucleotides flipped out to form base pairs with the neighboring nucleotides. Comparison of the A-DNA structure of the same sequence from two different crystal forms, reinforced the conclusion that molecules crystallized in the same space group have a more similar conformation, whereas the same molecule crystallized in different space groups has different (local) conformations.     

Amine free crystal structure: the crystal structure of d(CGCGCG)2 and methylamine complex crystal

We succeeded in the crystallization of d(CGCGCG)2 and methylamine Complex. The crystal was clear and of sufficient size to collect the X-ray crystallographic data up to 1.0 A resolution using synchrotron radiation. As a result of X-ray crystallographic analysis of 2Fo-Fc map was much clear and easily traced. It is the first time monoamine co-crystallizes with d(CGCGCG)2. However, methylamine was not found from the complex crystal of d(CGCGCG)2 and methylamine. Five Mg ions were found around d(CGCGCG)2 molecules. These Mg ions neutralized the anion of 10 values of the phosphate group of DNA with five Mg2+. DNA stabilized only by a metallic ion and there is no example of analyzing the X-ray crystal structure like this. Mg ion stabilizes the conformation of Z-DNA. To use monoamine for crystallization of DNA, we found that we can get only d(CGCGCG)2 and Mg cation crystal. Only Mg cation can stabilize the conformation of Z-DNA. The method of using the monoamine for the crystallization of DNA can be applied to the crystallization of DNA of long chain of length in the future like this.     

Cation-pi (Na+-Trp) interactions in the crystal structure of tetragonal lysozyme.

Experimental evidence of a cation-pi interaction between a sodium cation (Na+) and the indole ring of residue Trp123 in a structure (2.0 A) of hen egg-white lysozyme is presented. The geometry of the metal ion-pi interaction observed in the protein structure (distance between the aromatic plane and the cation approximately 4 A) is consistent with geometries observed among small molecules crystal structures and quantum chemistry ab initio calculations. The present crystal structure of lysozyme provides unique structural information about the geometry of binding of cations to pi systems in proteins. It shows that the metal ion-pi interaction within proteins is not significantly different from similar bindings found in small molecules and that it can be modeled by theoretical methods.     

The structure and hydration of the A-DNA fragment d(GGGTACCC) at room temperature and low temperature.

The DNA fragment d(GGGTACCC) was crystallized as an A-DNA duplex in the hexagonal space group P6(1). The structure was analyzed at room temperature and low temperature (100K) at a resolution of 2.5 A. The helical conformations at the two temperatures are similar but the low-temperature structure is more economically hydrated than the room-temperature one. The structure of d(GGGTACCC) is compared to those of d(GGGTGCCC) and d(GGGCGCCC). This series of molecules, which consists of a mismatched duplex and its two Watson-Crick analogues, exhibits three conformational variants of the A-form of DNA, which are correlated with the specific intermolecular interactions observed in the various crystals. The largest differences in local conformation are displayed by the stacking geometries of the central pyrimidine-purine and the flanking purine-pyrimidine sites in each of the three duplexes. Stacking energy calculations performed on the crystal structures show that the mismatched duplex is destabilized with respect to each of the error-free duplexes, in accordance with helix-coil transition measurements.     

High-resolution crystal structure of the intramolecular d(TpA) thymine-adenine photoadduct and its mechanistic implications

A high-resolution crystal structure is reported for d(TpA)*, the intramolecular thymine–adenine photoadduct that is produced by direct ultraviolet excitation of the dinucleoside monophosphate d(TpA). It confirms the presence of a central 1,3-diazacyclooctatriene ring linking the remnants of the T and A bases, as previously deduced from heteronuclear NMR measurements by Zhao et al. (The structure of d(TpA)*, the major photoproduct of thymidylyl-(3′-5′)-deoxyadenosine. Nucleic Acids Res., 1996, 24, 1554–1560). Within the crystal, the d(TpA)* molecules exist as zwitterions with a protonated amidine fragment of the eight-membered ring neutralizing the charge of the internucleotide phosphate monoanion. The absolute configuration at the original thymine C5 and C6 atoms is determined as 5S,6R. This is consistent with d(TpA)* arising by valence isomerization of a precursor cyclobutane photoproduct with cis–syn stereochemistry that is generated by [2 + 2] photoaddition of the thymine 5,6-double bond across the C6 and C5 positions of adenine. This mode of photoaddition should be favoured by the stacked conformation of adjacent T and A bases in B-form DNA. It is probable that the primary photoreaction is mechanistically analogous to pyrimidine dimerization despite having a much lower quantum yield.     

Crystal structure of the self-complementary 5''-purine start decamer d(GCACGCGTGC) in the A-DNA conformation. II.

The crystal structure of the alternating 5'-purine start decamer d(GCGCGCGCGC) was found to be in the left-handed Z-DNA conformation. Inasmuch as the A.T base pair is known to resist Z-DNA formation, we substituted A.T base pairs in the dyad-related positions of the decamer duplex. The alternating self-complementary decamer d(GCACGCGTGC) crystallizes in a different hexagonal space group, P6(1)22, with very different unit cell dimensions a = b = 38.97 and c = 77.34 A compared with the all-G.C alternating decamer. The A.T-containing decamer has one strand in the asymmetric unit, and because it is isomorphous to some other A-DNA decamers it was considered also to be right-handed. The structure was refined, starting with the atomic coordinates of the A-DNA decamer d(GCGGGCCCGC), by use of 2491 unique reflections out to 1.9-A resolution. The refinement converged to an R value of 18.6% for a total of 202 nucleotide atoms and 32 water molecules. This research further demonstrates that A.T base pairs not only resist the formation of Z-DNA but can also assist the formation of A-DNA by switching the helix handedness when the oligomer starts with a 5'-purine; also, the length of the inner Z-DNA stretch (d(CG)n) is reduced from an octamer to a tetramer. It may be noted that these oligonucleotide properties are in crystals and not necessarily in solutions.     

Crystal structure analysis of an A-DNA fragment at 1.8 A resolution: d(GCCCGGGC).

Single crystals of the self-complementary octadeoxyribonucleotide d(GCCCGGGC) have been analysed by X-ray diffraction methods at a resolution of 1.8 A. The tetragonal unit cell of space group P4(3)2(1)2 has dimensions of a = 43.25 A and c = 24.61 A and contains eight strands of the oligonucleotide. The structure was refined by standard crystallographic techniques to an R factor of 17.1% using 1359 3 sigma structure factor observations. Two strands of the oligonucleotide are related by the crystallographic dyad axis to form a DNA helix in the A conformation. The d(GCCCGGGC) helix is characterized by a wide open major groove, a near perpendicular orientation of base pairs to the helix axis and an unusually small average helix twist angle of 31.3 degrees indicating a slightly underwound helix with 11.5 base pairs per turn. Extensive cross-strand stacking between guanine bases at the central cytosine-guanine step is made possible by a number of local conformational adjustments including a fully extended sugar-phosphate backbone of the central guanosine nucleotide.     

The molecular structure of a 4'-epiadriamycin complex with d(TGATCA) at 1.7A resolution: comparison with the structure of 4'-epiadriamycin d(TGTACA) and d(CGATCG) complexes.

The structure of the complex between d(TGATCA) and the anthracycline 4'-epiadriamycin has been determined by crystallographic methods. The crystals are tetragonal, space group P4(1)2(1)2 with unit cell dimensions of a = 28.01, c = 52.95A. The asymmetric unit consists of one strand of hexanucleotide, one molecule of 4'-epiadriamycin and 34 waters. The R-factor is 20.2% for 1694 reflections with F greater than or equal to 2 sigma F to 1.7A. Two asymmetric units associate to generate a duplex complexed with two drug molecules at the d(TpG) steps of the duplex. The chromophore intercalates between these base pairs with the anthracycline amino-sugar positioned in the minor groove. The double helix is a distorted B-DNA type structure. Our structure determination of d(TGATCA) complexed to 4'-epiadriamycin allows for comparison with the previously reported structures of 4'-epiadriamycin bound to d(TGTACA) and to d(CGATCG). The three complexes are similar in gross features and the intercalation geometry is the same irrespective of whether a d(CpG) or d(TpG) sequence is involved. However, the orientation of the amino-sugar displays a dependence on the sequence adjacent to the intercalation site. The flexibility of this amino-sugar may help explain why this class of antibiotics displays a relative insensitivity to base sequence when they bind to DNA.     

Relationship of DNA structure to internal dynamics: correlation of helical parameters from NOE-based NMR solution structures of d(GCGTACGC)(2) and d(CGCTAGCG)(2) with (13)C order parameters implies conformational coupling in dinucleotide units

The coupling between the conformational properties of double-stranded DNA and its internal dynamics has been examined. The solution structures of the isomeric DNA oligomers d(GCGTACGC)(2) (UM) and d(CGCTAGCG)(2) (CTSYM) were determined with (1)H NMR spectroscopy by utilizing distance restraints from total relaxation matrix analysis of NOESY cross-peak intensities in restrained molecular dynamics calculations. The root-mean-square deviation of the coordinates for the ensemble of structures was 0.13 A for UM and 0.49 A for CTSYM, with crystallographic equivalent R(c)=0.41 and 0.39 and sixth-root residual R(x)=0.11 and 0.10 for UM and CTSYM, respectively. Both UM and CTSYM are B-form with straight helical axes and show sequence-dependent variations in conformation. The internal dynamics of UM and CTSYM were previously determined by analysis of (13)C relaxation parameters in the context of the Lipari & Szabo model-free formalism. Helical parameters for the two DNA oligomers were examined for linear correlations with the order parameters (S(2)) of groups of (13)C spins in base-pairs and dinucleotide units of UM and CTSYM. Correlations were found for six interstrand base-pair parameters tip, y-displacement, inclination, buckle and stretch with various combinations of S(2) for atoms in Watson-Crick base-pairs and for two inter-base-pair parameters, rise and roll with various combinations of S(2) for atoms in dinucleotides. The correlations for the interstrand base-pair helical parameters indicate that the conformations of the deoxyribose residues of each strand are dynamically coupled. Also, the inter-base-pair separation has a profound effect on the local internal motions available to the DNA, supporting the idea that rise is a principal degree of freedom for DNA conformational variability. The correlations indicate collective atomic motions of spins that may represent specific motional modes in DNA, and that base sequence has a predictable effect on the relative order of groups of spins both in the bases and in the deoxyribose ring of the DNA backbone. These observations suggest that an important functional outcome of DNA base sequence is the modulation of both the conformation and dynamic behavior of the DNA backbone.     

Crystal structure at 1.5-A resolution of d(CGCICICG), an octanucleotide containing inosine, and its comparison with d(CGCG) and d(CGCGCG) structures.

The octadeoxyribonucleotide d(CGCICICG) has been crystallized in space group P(6)5(22) with unit cell dimensions of a = b = 31.0 A and c = 43.7 A, and X-ray diffraction data have been collected to 1.5-A resolution. Precession photographs and the self-Patterson function indicate that 12 base pairs of Z-conformation DNA stack along the c-axis, and the double helices pack in a hexagonal array similar to that seen in other crystals of Z-DNA. The structure has been solved by both Patterson deconvolution and molecular replacement methods and refined in space group P(6)5 to an R factor of 0.225 using 2503 unique reflections greater than 3.0 sigma (F). Comparison of the molecules within the hexagonal lattice with highly refined crystal structures of other Z-DNA reveals only minor conformational differences, most notably in the pucker of the deoxyribose of the purine residues. The DNA has multiple occupancy of C:I and C:G base pairs, and C:I base pairs adopt a conformation similar to that of C:G base pairs.     

The structure of a full turn of an A-DNA duplex d(CGCGGGTACCCGCG)2

We report the 2.6 Å resolution crystal structure of the tetra-decamer d(CGCGGGTACCCGCG) in the tetragonal space group P4₃. This sequence contains the KpnI restriction site GGTACC in the centre which is flanked by alternating ‘CG’ sequences, and has a ‘TA’ step at the centre. These are features could favour the left-handed Z type helix. Despite this, overall the molecule has the A form. This is the first tetra-decamer crystallized in the A-DNA conformation, i.e. more than one full turn of the A helix. The crystallographic asymmetric unit consists of one tetra-decamer duplex. The helical twist and slide, as well as the base pair–base pair stacking interactions show alternations at the alternating pyrimidine–purine and purine–pyrimidine base steps. This variation is reminiscent of the dinucleotide repeat in left-handed Z-DNA helices. The crystal packing is unlike other A-DNA crystal structures, with each helix having a large number of contacts of many different types with symmetry-related neighbours.     

DNA-drug interactions. The crystal structure of d(CGATCG) complexed with daunomycin

The structure of a d(CGATCG)-daunomycin complex has been determined by single crystal X-ray diffraction techniques. Refinement, with the location of 40 solvent molecules, using data up to 1.5 A, converged with a final crystallographic residual, R = 0.25 (RW = 0.22). The tetragonal crystals are in space group P4(1)2(1)2, with cell dimensions of a = 27.98 A and c = 52.87 A. The self-complementary d(CGATCG) forms a distorted right-handed helix with a daunomycin molecule intercalated at each d(CpG) step. The daunomycin aglycon chromophore is oriented at right-angles to the long axis of the DNA base-pairs. This head-on intercalation is stabilized by direct hydrogen bonds and indirectly via solvent-mediated, hydrogen-bonding interactions between the chromophore and its intercalation site base-pairs. The cyclohexene ring and amino sugar substituent lie in the minor groove. The amino sugar N-3' forms a hydrogen bond with O-2 of the next neighbouring thymine. This electrostatic interaction helps position the sugar in a way that results in extensive van der Waals contacts between the drug and the DNA. There is no interaction between daunosamine and the DNA sugar-phosphate backbone. We present full experimental details and all relevant conformational parameters, and use the comparison with a d(CGTACG)-daunomycin complex to rationalize some neighbouring sequence effects involved in daunomycin binding.     

Crystal and molecular structure of d(GTGCGCAC): investigation of the effects of base sequence on the conformation of octamer duplexes.

The structure of the self-complementary deoxyoctanucleotide d(GTGCGCAC), which crystallized as an A-type helix in the space group P4(3)2(1)2, with one strand in the crystallographic asymmetric unit has been determined and refined to a final R-value of 0.154 using 1.64-A diffraction data collected on an area detector. In contrast to the closely related sequence d(GTGTACAC)tet, there was no evidence for an ordered spermine molecule in the major groove of this octamer. Ordered water is found associated with almost all the exposed hydrogen bonding groups of the octamer. A pentagonal ring of water molecules is hydrogen bonded to O6 and N7 of G3 and the N4 and O6 of the C4.G13 base pair. A detailed comparison of the local helical parameters of d(GTGCGCAC) and d(GTGTACAC)tet is presented. The base sequence change at the center of the octamers affects several of the local helical parameters, via both intra- and interduplex interactions within the crystal.     

Cobalt hexammine induced tautomeric shift in Z-DNA: the structure of d(CGCGCA)*d(TGCGCG) in two crystal forms

We report here the crystal structure of the DNA hexamer duplex d(CGCGCA).d(TGCGCG) at 1.71 Å resolution. The crystals, in orthorhombic space group, were grown in the presence of cobalt hexammine, a known inducer of the left-handed Z form of DNA. The interaction of this ion with the DNA helix results in a change of the adenine base from the common amino tautomeric form to the imino tautomer. Consequently the A:T base pair is disrupted from the normal Watson–Crick base pairing to a ‘wobble’ like base pairing. This change is accommodated easily within the helix, and the helical parameters are those expected for Z-DNA. When the cobalt hexammine concentration is decreased slightly in the crystallization conditions, the duplex crystallizes in a different, hexagonal space group, with two hexamer duplexes in the asymmetric unit. One of these is situated on a crystallographic 6-fold screw axis, leading to disorder. The tautomeric shift is not observed in this space group. We show that the change in inter-helix interactions that lead to the two different space groups probably arise from the small decrease in ion concentration, and consequently disordered positions for the ion.