Lucy Malinina

Water and Ions in a High Resolution Structure of B-DNA

A detailed picture of hydration and counterion location in the B-DNA duplex d(GCGAATTCG) is presented. Detailed data have been obtained by single crystal x-ray diffraction at atomic resolution (0.89 Å) in the presence of Mg2+. The latter is the highest resolution ever obtained for a B-DNA oligonucleotide. Minor groove hydration is compared with that found in the Na+ and Ca2+ crystal forms of the related dodecamer d(CGCGAATTCGCG). High resolution data (1.45 Å) of the Ca2+ form obtained in our laboratory are used for that purpose. The central GAATTC has a very stable hydration spine identical in all cases, independent of duplex length and crystallization conditions (counterions, space group). However, the organization of the water molecules (tertiary and quaternary layers) associated with the central spine vary in each case.

Solvent Organization in an Oligonucleotide Crystal THE STRUCTURE OF d(GCGAATTCG)2 AT ATOMIC RESOLUTION

We describe the crystal structure of d(GCGAATTCG) determined by x-ray diffraction at atomic resolution level (0.89 Å). The duplex structure is practically identical to that described at 2.05 Å resolution (Van Meervelt, L., Vlieghe, D., Dautant, A., Gallois, B., Précigoux, G., and Kennard, O. (1995) Nature 374, 742–744), however about half of the phosphate groups show multiple conformations. The crystal has three regions with different solvent structure. One of them contains several ordered Mg+2 ions and can be considered as an ionic crystal. A second region is formed by a network of ordered water molecules with a polygonal organization that binds three duplexes. The third region is formed by channels of solvent in which very few ordered solvent molecules are visible. The less ordered phosphates are found facing this channel. The latter region provides a view of DNA with highly movable charges, both negative phosphates and counterions, without a precise location.

The structure of the most studied DNA fragment changes under the influence of ions: a new packing of d(CGCGAATTCGCG)

The title oligonucleotide and many related dodecamers have been extensively studied alone and as DNA‐drug complexes. In practically all cases they were found to crystallize in the same space group, stabilized by interactions among the terminal guanine bases. Here we report new packing interactions (R3) in the presence of Ca2+. The oligonucleotides interact by placing their terminal guanines in the narrow groove of a neighbor molecule, an interaction which had never been found in dodecamers.

STRUCTURAL VARIABILITY AND NEW INTERMOLECULAR INTERACTIONS OF Z-DNA IN CRYSTALS OF D(PCPGPCPGPCPG)

We have determined the single crystal x-ray structure of the synthetic DNA hexamer d(pCpGpCpGpCpG) in two different crystal forms. The hexamer pCGCGCG has the Z-DNA conformation and in both cases the asymmetric unit contains more than one Z-DNA duplex. Crystals belong to the space group C222(1) with a = 69.73, b = 52.63, and c = 26.21 A, and to the space group P2(1) with a = 49.87, b = 41.26, c = 21.91 A, and gamma = 97.12 degrees. Both crystals show new crystal packing modes. The molecules also show striking new features when compared with previously determined Z-DNA structures: 1) the bases in one duplex have a large inclination with respect to the helical axis, which alters the overall shape of the molecule. 2) Some cytosine nitrogens interact by hydrogen bonding with phosphates in neighbor molecules. Similar base-phosphate interactions had been previously detected in some B-DNA crystals. 3) Basepair stacking between the ends of neighbor molecules is variable and no helical continuity is maintained between contiguous hexamer duplexes.

Structural variability of A-DNA in crystals of the octamer d(pCpCpCpGpCpGpGpG)

We have determined the structure of the synthetic DNA octamer d(pCpCpCpGpCpGpGpG) in five different crystal forms by single crystal X-ray diffraction. One crystal belongs to the space group P4(3)2(1)2 with a = b = 41.77, c = 25.15 A, whereas all others have the space group P2(1)2(1)2(1) with progressively decreasing unit cell volumes. In all crystals the octamer forms duplexes of A-DNA and all crystals display a similar packing mode, typical for A-DNA. The structure of the duplex varies from loose to very compact when going from one crystal form to another. The most compact form exhibits a volume of 995 A3 per base pair. Such a high density has never been found in A-DNA, being more characteristic of Z-DNA crystals. A comparison of the most with the least compact forms gives a RMS value of 1.7 A, with the distance between the phosphate centers through the major groove being almost twice shorter in the compact form. The phosphate-phosphate separation across the major groove in the compact form is extremely small, 0.7 A. The helical parameters also vary significantly in the various crystal forms. Differences in the helical twist can reach 13 degrees in the same step of the octamer in different crystal forms. The results prove that A-DNA is structurally very variable and demonstrate that the local structure of the same DNA fragment can strongly depend on the crystal environment.

Phase Diagrams for DNA Crystallization Systems

Phase diagrams for several oligonucleotide duplex-spermine systems have been constructed. These diagrams characterize the duplex and spermine concentrations ranges in which crystalline precipitates are formed. All of them are wedge-like form. The slope of the upper branch of the diagram is determined by the oligonucleotide length. The position of the lower branch depends on both the nucleotide sequence and its length. The position of the lower branch depends on both the nucleotide sequence and its length. It has been shown that the addition to the system of MgCl2 and NaCl salts and MPD results in specific changes in the diagrams. A model for oligonucleotide duplex-spermine system has been suggested which explains the main characteristic features of the obtained phase diagrams. The experimental phase diagrams for the (pGpT)n (pApC)n-spermine system (n = 2,3,4) have been analyzed ion terms of this model and the values of the binding constants of spermine and Mg2+ ions binding to duplexes have been determined. It permitted to identify the complexes that precipitated in different regions of the phase diagrams under various conditions. The diagram obtained in the presence of a cobalt hexammine counterion is also considered. It has been shown that this phase diagram, in general, is similar to those obtained for the oligonucleotide duplex-spermine system.

A Simplified Multidimensional Search Used For Crystal Structure Solution of pCpGpCpGpCpG With Two Duplexes per Asymmetric Unit

A simplified multidimensional search was applied to determine the structure of deoxyhexamer CGCGCG in the crystal form belonging to the space group C222(1) (a = 45.6 A, b = 37.3 A, c = 70.3 A). This crystal form contains two Z-DNA duplexes per asymmetric unit in a similar orientation. The search consists of several main steps. As a first step, the analysis of packing modes is carried out and constraints for the position of duplexes in asymmetric unit are formulated. In order to choose true packing mode duplexes are represented as cylinders of a constant density and global search is carried out. Only reflections belonging to the plane in reciprocal space perpendicular to DNA axis were used in the calculations. An analytical representation of diffraction from a hollow cylinder is given which allows further refinement of corresponding parameters. During the global search the value of a linear correlation coefficient is estimated for each solution to pick up the best one. At the second step the more local search is carried out. The DNA model of a certain conformation (in our case Z-DNA) is taken and several parameters are being varied. These are: a) rotations of the independent duplexes around their axes (only two rotational parameters for two duplexes in our example) and b) a few positional parameters for which there is no corresponding constraint in the packing mode tested. In our case we had to vary only x1 and y2, where subindex corresponds to molecule number. The last stage concerned is quite similar to the multidimensional search realised in program ULTIMA. The only difference that the number of variable parameters is less in our search. This number for the case under consideration was 4 instead of 12 that would be necessary in a conventional multidimensional search.

An efficient and possibly general packing mode for crystals of B-DNA oligonucleotides

Two crystal forms of the self-complementary deoxytetramer GpGpCpC have been obtained by use of the phase diagram technique: hexagonal P6222 or P6422 witha =b = 67.7A˚,c = 105.6A˚, and trigonal P3212 or P3112 witha =b = 116.9A˚,c = 116.4A˚. Diffraction patterns from both crystals show strong 3.38A˚reflections that are typical of base-stacking in B-DNA. The self-rotation functionR(ϕ, ψ, 180°) for the hexagonal form exhibits peaks representing pseudodyad rotation, whose periodicity also suggests B-DNA. Crystal packing arguments also favor use of this crystal form for a B helix.

DNA MOBILITY IN CRYSTALS OF A NONSPECIFIC LAMBDA CRO/DNA COMPLEX

DNA location in the crystal of the nonspecific lambda cro/(GT)4.(AC)4 complex has been studied by the isomorphous replacement method using iodinated and brominated oligonucleotides. The results of the search for heavy atom positions combined with previously obtained molecular replacement data suggest that the DNA octamer occupies two overlapping positions, each of the two duplexes (GTGTGTGT).(ACACACAC) belonging to the same imaginary longer double helix and differing only in the shift by two base pairs along the common sugar-phosphate backbone. In the crystals of the heavy atom derivatives different orientations of the DNA octamer are observed as well. It seems reasonable that the DNA mobility of both kinds might be a common feature of crystals of nonspecific repressor/DNA complexes.