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.     

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 the complex of Hoechst 33258 and the DNA dodecamer d(CGCGAATTCGCG).

The crystal structure of the complex between the dodecamer d(CGCGAATTCGCG) and a synthetic dye molecule Hoechst 33258 was solved by X-ray diffraction analysis and refined to an R-factor of 15.7% at 2.25 A resolution. The crescent-shaped Hoechst compound is found to bind to the central four AATT base pairs in the narrow minor groove of the B-DNA double helix. The piperazine ring of the drug has its flat face almost parallel to the aromatic bisbenzimidazole ring and lies sideways in the minor groove. No evidence of disordered structure of the drug is seen in the complex. The binding of Hoechst to DNA is stabilized by a combination of hydrogen bonding, van der Waals interaction and electrostatic interactions. The binding preference for AT base pairs by the drug is the result of the close contact between the Hoechst molecule and the C2 hydrogen atoms of adenine. The nature of these contacts precludes the binding of the drug to G-C base pairs due to the presence of N2 amino groups of guanines. The present crystal structural information agrees well with the data obtained from chemical footprinting experiments.     

Crystal and molecular structure of a DNA fragment: d(CGTGAATTCACG)

The crystal structure of the dodecanucleotide d(CGTGAATTCACG) has been determined to a resolution of 2.7 A and refined to an R factor of 17.0% for 1532 reflections. The sequence crystallizes as a B-form double helix, with Watson-Crick base pairing. This sequence contains the EcoRI restriction endonuclease recognition site, GAATTC, and is flanked by CGT on the 5'-end and ACG on the 3'-end, in contrast to the CGC on the 5'-end and GCG on the 3'-end in the parent dodecamer d(CGCGAATTCGCG). A comparison with the isomorphous parent compound shows that any changes in the structure induced by the change in the sequence in the flanking region are highly localized. The global conformation of the duplex is conserved. The overall bend in the helix is 10 degrees. The average helical twist values for the present and the parent structures are 36.5 degrees and 36.4 degrees, respectively, corresponding to 10 base pairs per turn. The buckle at the substituted sites are significantly different from those seen at the corresponding positions in the parent dodecamer. Step 2 (GpT) is underwound with respect to the parent structure (27 degrees vs 36 degrees) and step 3 (TpG) is overwound (34 degrees vs 27 degrees). There is a spine of hydration in the narrow minor groove. The N3 atom of adenine on the substituted A10 and A22 bases are involved in the formation of hydrogen bonds with other duplexes or with water; the N3 atom of guanine on G10 and G22 bases in the parent structure does not form hydrogen bonds.     

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.     

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 the B-DNA dodecamer CGTGAATTCACG.

The crystal structure of the DNA dodecamer C-G-T-G-A-A-T-T-C-A-C-G has been determined at a resolution of 2.5 A, with a final R factor of 15.8% for 1475 nonzero reflections measured at 0 degrees C. The structure is isomorphous with that of the Drew dodecamer, with the space group P2(1)2(1)2(1) and cell dimensions of a = 24.94 A, b = 40.78 A, and c = 66.13 A. The asymmetric unit contains all 12 base pairs of the B-DNA double helix and 36 water molecules. The structure of C-G-T-G-A-A-T-T-C-A-C-G is very similar to that of C-G-C-G-A-A-T-T-C-G-C-G, with no major alterations in helix parameters. Water peaks in the refined structure appear to represent a selection of peaks that were observed in the Drew dodecamer. The minor-groove spine of hydration at 2.5 A is fragmentary, but as Narendra et al. (1991) [Biochemistry (following paper in this issue)] have observed, lowering the temperature leads to a more complete representation of the spine.     

The 31P-NMR spectrum of the dodecamer d(GACGATATCGTC).

The resonances in the 31P-NMR spectrum of the dodecamer d(GACGATATCGTC) have been assigned by regiospecific labelling with oxygen-17. All 11 resonances are clearly resolved at 26 degrees C. Most noticeably, individual resonances of the dinucleoside phosphates d(CpG), d(TpC), d(GpA) and d(ApT) which occur more than once can clearly be distinguished. This indicates that the position of the phosphate group in the oligomer influences its 31P-NMR shift. This observation is in agreement with what has been found for the 31P-NMR spectra of d(CGCGAATTCGCG) [Ott, J. and Eckstein, F. (1985) Biochemistry 24] and d(GGAATTCC) [Connolly, B.A. and Eckstein, F. (1984) Biochemistry 23, 5523-5527]. In general, the chemical shift appears the more at higher field the more central the dinucleoside phosphate is located in the oligomer. Exceptions are the resonances of dinucleoside phosphates of the type 5'-PyPu-3' which appear at lower field than expected from this rule. A reasonable correlation between 31P-NMR chemical shifts and the sum function of the base plane roll angles derived from Calladine's rule [Calladine, C.R. (1982) J. Mol. Biol. 161, 343-352] exists.     

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.     

Hexagonal crystal structure of the A-DNA octamer d(GTGTACAC) and its comparison with the tetragonal structure: correlated variations in helical parameters

The alternating DNA octamer d(GTGTACAC) has been grown in a novel hexagonal crystal form. The structure has been determined and refined to a 2-A resolution, with 51 water molecules. The A-DNA conformation is a variant of that observed for the tetragonal form of the same sequence (Jain et al., 1989) containing a bound spermine. The crystals belong to the space group P6(1)22, a = b = 32.40 A and c = 79.25 A, with one strand in the asymmetric unit. The new hexagonal structure was solved by rotation and translation searches in direct space and refined to a final R value of 12.7% by using 1561 unique reflections greater than 1.5 sigma (I). The electron density clearly shows that the penultimate A7 sugar had flipped into the alternative C2'-endo pucker. This dent in the molecule can be attributed to close intermolecular contacts. In contrast, in the tetragonal structure, the DNA is distorted in the central TA step, where the A5 backbone bonds C4'-C5' and O5'-P assume trans conformations. The hexagonal double helix more closely resembles the fiber diffraction A-DNA, compared to the tetragonal form. For instance, the tilt angle is higher (16 degrees vs 10 degrees), which is correlated with a larger displacement from the helix axis (3.5 vs 3.3), a lower rise per residue (2.9 vs 3.2), and a smaller major-groove width (6.1 vs 8.7), thus indicating that the variations in these global helical parameters are correlated. The propeller twist angles in both forms are higher for the G-C base pairs (15.3 degrees, 12.14 degrees) than for the A-T base pairs (10.8 degrees, 9.1 degrees), which is the reverse of the expected order. Unlike the tetragonal structure, the hexagonal crystal structure interestingly does not contain a bound spermine molecule. Our analysis reveals that the conformational differences between the tetragonal and hexagonal forms are not entirely due to the spermine binding, and crystal packing seems to play an important role.     

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 ammonium salt of the dinucleoside monophosphate d(CpG)

The crystal and molecular structure of the ammonium salt of deoxycytidylyl-(3'-5')-deoxyguanosine has been determined from 0.85 A resolution single crystal X-ray diffraction data. The crystals obtained by acetone diffusion technique at -20 degrees C, are orthorhombic, P212121, a = 12.880(2), b = 17444(2) and c = 27.642(2) A. The structure was solved by high resolution Patterson and Fourier methods and refined to R = 0.136. There are two d(CpG) molecules in the asymmetric unit forming a mini left handed Z-DNA helix. This is in contrast to the earlier reported forms of d(CpG) where the molecules form self base paired duplexes. There are two ammonium ions in the asymmetric unit. The major groove NH+4 ion interacts with N7 of guanines through water bridges besides making H-bonded interactions directly with the phosphate oxygen atoms. A second NH+4 ion is found in the minor groove interacting directly with the phosphate oxygen atoms. Symmetry related molecules pack in such a way that the cytosine base stacks on cytosine and guanine base on guanine. Our structure demonstrates that alternating d(CpG) sequences have the ability to adopt the left handed Z-DNA structure even at the dimer level i.e., in a sequence which is only two base pairs long.     

Crystal and molecular structure of the sodium salt of the dinucleotide duplex d(CpG)

The crystal and molecular structure of the sodium salt of deoxycytidylyl-(3H-5H)-deoxyguanosine has been determined from X-ray diffraction data. The crystal, obtained from an aqueous gamma-butyrolactone solution at pH = 5.3 are orthorhombic, P212121, a = 10.640(2), b = 11.184(2) and c = 44.618(4)A. The structure was refined to an R = 0.041. The d(CpG) structure is similar to the ammonium salt solved by Cruse et al.(1). Both structures form a parallel self base paired mini-double helix. In d(CpG).Na+ one of the two paired cytosines is protonated on N(3). The cytosines form 3 hydrogen bonds while the guanines form only 2. The Na+ ion is coordinated with five groups: two water molecules, O(6) of guanine A, N(7) of guanine B and 0(5') of cytosine B, forming a square pyramid. The hydration shell around the mini-helix is analysed and compared with that of the ammonium salt, d(CpG).Na+ is the second d(CpG) oligonucleotide found with a self base pairing arrangement despite of the fact that the crystallization conditions and counterion were different in both cases. The hypothesis that self base pairing is not only a crystallization artifact but may play a role under physiological conditions as a source of transversion mutations is discussed.     

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.     

Crystal structure of a B-DNA dodecamer containing inosine, d(CGCIAATTCGCG), at 2.4 A resolution and its comparison with other B-DNA dodecamers.

The crystal structure of the dodecamer, d(CGCIAATTCGCG), has been determined at 2.4 A resolution by molecular replacement, and refined to an R-factor of 0.174. The structure is isomorphous with that of the B-DNA dodecamer, d(CGCGAATTCGCG), in space group P2(1)2(1)2(1) with cell dimensions of a = 24.9, b = 40.4, and c = 66.4 A. The initial difference Fourier maps clearly indicated the presence of inosine instead of guanine. The structure was refined with 44 water molecules, and compared to the parent dodecamer. Overall the two structures are very similar, and the I:C forms Watson-Crick base pairs with similar hydrogen bond geometry to the G:C base pairs. The propeller twist angle is low for I4:C21 and relatively high for the I16:C9 base pair (-3.2 degrees compared to -23.0 degrees), and the buckle angles alter, probably due to differences in the contacts with symmetry related molecules in the crystal lattice. The central base pairs of d(CGCIAATTCGCG) show the large propeller twist angles, and the narrow minor groove that characterize A-tract DNA, although I:C base pairs cannot form the major groove bifurcated hydrogen bonds that are possible for A:T base pairs.     

Solution structure of the dodecamer d-(CATGGGCC-CATG)2 is B-DNA. Experimental and molecular dynamics study

The DNA duplex d-(CATGGGCCCATG)2 has been studied in solution by FTIR, NMR and CD. The experimental approaches have been complemented by series of large-scale unrestrained molecular dynamics simulation with explicit inclusion of solvent and counterions. Typical proton-proton distances extracted from the NMR spectra and the CD spectra are completely in agreement with slightly modified B-DNA. By molecular dynamics simulation, starting from A-type sugar pucker, a spontaneous repuckering to B-type sugar pucker was observed. Both experimental and theoretical approaches suggest for the dodecamer d-(CATGGGCCCATG)2 under solution conditions puckering of all 2'-deoxyribose residues in the south conformation (mostly C2'-endo) and can exclude significant population of sugars in the north conformation (C3'-endo). NMR, FTIR and CD data are in agreement with a B-form of the dodecamer in solution. Furthermore, the duplex shows a cooperative B-A transition in solution induced by addition of trifluorethanol. This contrasts a recently published crystal structure of the same oligonucleotide found as an intermediate between B- and A-DNA where 23 out of 24 sugar residues were reported to adopt the north (N-type) conformation (C3'-endo) like in A-DNA (Ng, H. L., Kopka, M. L. and Dickerson, R. E., Proc. Natl. Acad. Sci. U S A 97, 2035-2039 (2000)). The simulated structures resemble standard B-DNA. They nevertheless show a moderate shift towards A-type stacking similar to that seen in the crystal, despite the striking difference in sugar puckers between the MD and X-ray structures. This is in agreement with preceding MD reports noticing special stacking features of G-tracts exhibiting a tendency towards the A-type stacking supported by the CD spectra also reflecting the G-tract stacking. MD simulations reveal several noticeable local conformational variations, such as redistribution of helical twist and base pair roll between the central GpC steps and the adjacent G-tract segments, as well as a substantial helical twist variability in the CpA(TpG) steps combined with a large positive base pair roll. These local variations are rather different from those seen in the crystal.     

The molecular structure of Okazaki fragment r(CGCA)d(AAAAAGCG):d(CGCTTTTTTGCG) in solution

The hetero duplex molecule, r(CGCA)d(AAAAAGCG):d(CGCTTTTTTGCG) which corresponds to Okazaki fragment was synthesized and its molecular structure has been analyzed by NMR study. The RNA strand of RNA-DNA hybrid region adopts A-form and DNA strand of the same region deviates from the standard B-form. The conformation of DNA-DNA duplex segment belongs to B-form. The hybrid-DNA duplex junction shows a structural discontinuities, A-B junction. The same conformational characteristic of oligo(dA): oligo(dT) tract as that of DNA oligomer which has same base sequence has been observed.     

Crystal and solution structures of the B-DNA dodecamer d(CGCAAATTTGCG) probed by Raman spectroscopy: heterogeneity in the crystal structure does not persist in the solution structure

The self-complementary dodecamer d(CGCAAATTTGCG) crystallizes as a double helix of the B form and manifests a Raman spectrum with features not observed in Raman spectra of either DNA solutions or wet DNA fibers. A number of Raman bands are assigned to specific nucleoside sugar and phosphodiester conformations associated with this model B-DNA crystal structure. The Raman bands proposed as markers of the crystalline B-DNA structure are compared and contrasted with previously proposed markers of Z-DNA and A-DNA crystals. The results indicate that the three canonical forms of DNA can be readily distinguished by Raman spectroscopy. However, unlike Z-DNA and A-DNA, which retain their characteristic Raman fingerprints in aqueous solution, the B-DNA Raman spectrum is not completely conserved between crystal and solution states. The Raman spectra reveal greater heterogeneity of nucleoside conformations (sugar puckers) in the DNA molecules of the crystal structure than in those of the solution structure. The results are consistent with conversion of one-third of the dG residues from the C2'-endo/anti conformation in the solution structure to another conformation, deduced to be C1'-exo/anti, in the crystal. The dodecamer crystal also exhibits unusually broad Raman bands at 790 and 820 cm-1, associated with the geometry of the phosphodiester backbone and indicating a wider range of (alpha, zeta) backbone torsion angles in the crystal than in the solution structure. The results suggest that backbone torsion angles in the CGC and GCG sequences, which flank the central AAATTT sequence, are significantly different for crystal and solution structures, the former containing the greater diversity.(ABSTRACT TRUNCATED AT 250 WORDS)