No abstract

The widely used antitumor drug cis-diamminedichloroplatinum(II) (cisplatin or cis-DDP) reacts with DNA, cross-linking two purine residues through the N7 atoms, which reside in the major groove in B-form DNA. The solution structure of the short duplex [d(CAT-AGCTATG)]2 cross-linked at the GC:GC site was determined by nuclear magnetic resonance (NMR). The deoxyguanosine-bridging cis-diammineplatinum(II) lies in the minor groove, and the complementary deoxycytidines are extrahelical. The double helix is locally reversed to a left-handed form, and the helix is unwound and bent toward the minor groove. These findings were independently confirmed by results from a phase-sensitive gel electrophoresis bending assay. The NMR structure differs markedly from previously proposed models but accounts for the chemical reactivity, the unwinding, and the bending of cis-DDP interstrand cross-linked DNA and may be important in the formation and repair of these cross-links in chromatin.

No abstract

In DNA or RNA duplexes, the six-bond C3'-O3'-P-O5'-C5'-C4'-C3' backbone linkage connecting adjacent residues contains six torsion angles (epsilon, zeta, alpha, beta, gamma, delta) but only four protons. This seriously limits the ability to define the backbone conformation by NMR using purely 1H-1H distance geometry (DG) methods. The problem is further compounded by the inability to assign two of the four backbone protons, namely the poorly resolved H5' and H5'' protons, and invariably leads to DG structures with poorly defined backbone conformations. We have developed and tested a reliable method to constrain the beta, gamma, and epsilon (and indirectly alpha and zeta) backbone torsion angles by lower-bound NOE distances to unassigned H5'/H5'' resonances combined with either 1H line widths or the conservative use of sigma J measurements; the method relies only on 1H 2-D NMR data, does not involve any structural assumptions, and leads to much improved backbone convergence among DG structures. The C4'-C5' torsion angle gamma is constrained by lower-bound NOE distances from H2' and from H6/H8 to any H5'/H5'', as well as by sigma JH4, coupling measurements in the 3.9-4.4 ppm region; delta is constrained by H1'-H4' NOE distances and by H3'-H4' and H3'-H2'' J couplings in COSY data; epsilon is partially constrained by H3' line width and/or further constrained by subtracting the minimum possible sigma JH3'-H from the observed sigma JH3' (COSY) to arrive at the maximum possible JH3'-P, which is then converted to H3'-P distance bounds. The angle beta is partially constrained via H5'-P and H5''-P distance bounds consistent with the maximum H5'-P and H5''-P J couplings derived from the observed H5' and H5'' line widths, while alpha and zeta are indirectly constrained by lower distance bounds on the observed (n)H1' to (n + 1)H5'/H5'' NOEs combined with the prior partial constraints on beta, gamma, delta, and epsilon. The combined effects of these additional constraints in determining distance geometry structures have been demonstrated using a 12-base duplex, [d(GCCGTTAACGGC)]2. Coordinate RMSDs per atom between structures refined with these constraints from random-embedded DG structures, from ideal A-DNA, and from B-DNA starting structures were less than 0.4 A for the central 8 base pairs indicating good convergence. All backbone angles for the central 8 base pairs are very well constrained with less than 10 degrees variation in any of the 48 torsion angles.

The three-dimensional structure of d(CGCGTTTTCGCG) in solution has been determined from proton NMR data by using distance geometry methods. The rate of dipolar cross-relaxation between protons close together in space is used to calculate distances between proton pairs within 5 A of each other; these distances are used as input to a distance geometry algorithm that embeds this distance matrix in three-dimensional space. The resulting refined structures that best agree with the input distances are all very similar to each other and show that the DNA sequence forms a hairpin in solution; the bases of the loop region are stacked, and the stem region forms a right-handed helix. The advantages and limitations of the technique, as well as the computer requirements of the algorithm, are discussed.

High-resolution NMR techniques have been used to examine the structural and dynamical features of the interaction between distamycin A and the self-complementary DNA dodecamer duplex d-(CGCGAATTCGCG)2. The proton resonances of d(CGCGAATTCGCG)2 have been completely assigned by previous two-dimensional NMR studies [Hare, D. R., Wemmer, D. E., Chou, S. H., Drobny, G., & Reid, B. R. (1983) J. Mol. Biol. 171, 319-336]. Addition of the asymmetric drug molecule to the symmetric dodecamer leads to the formation of an asymmetric complex as evidenced by a doubling of DNA resonances over much of the spectrum. In two-dimensional exchange experiments, strong cross-peaks were observed between uncomplexed DNA and drug-bound DNA resonances, permitting direct assignment of many drug-bound DNA resonances from previously assigned free DNA resonances. Weaker exchange cross-peaks between formerly symmetry related DNA resonances indicate that the drug molecule flips head-to-tail on one duplex with half the frequency at which it leaves the DNA molecule completely. In experiments performed in H2O, nuclear Overhauser effects (NOEs) were observed from each drug amide proton to an adenine C2H and a pyrrole H3 ring proton. In two-dimensional nuclear Overhauser experiments performed on D2O solutions, strong intermolecular NOEs were observed between each of the three pyrrole H3 resonances of the drug and an adenine C2H resonance, with weaker NOEs observed between the drug H3 resonances and C1'H resonances. The combined NOE data allow us to position the distamycin A unambiguously on the DNA dodecamer, with the drug spanning the central AATT segment in the minor groove.

There has been a surge of recent interest, reflected by a sharp increase in the number of publications, in the area of high-resolution nuclear magnetic resonance (NMR) studies of DNA. The goal of many of these studies is to monitor the structure of biologically important DNA sequences directly in solution; the impetus for such studies was the realization, from early single-crystal X-ray structures, that nearest-neighbor context effects are a major determinant of local structure in short double-helical DNAs (Dickerson & Drew, 1981; Dickerson, 1983). Thus, instead of the previously assumed regular averaged structure of the double helix derived from fibre diffraction analysis, the more interesting concept emerged that specific sequence-dependent distortions from ‘classical’ DNA structure might be responsible for the recognition of such sequences by a variety of ligands such as repressors, polymerases, drugs, etc.

The solution structure of the self-complementary DNA duplex [d(CGCGAATTCGCG)]2, which contains the EcoRI restriction site sequence GAATTC at the center, has been studied by two-dimensional nuclear magnetic resonance spectroscopy. Time-dependent nuclear Overhauser effect spectra were used to obtain the initial cross-relaxation rates between 155 pairs of protons. These initial cross-relaxation rates were converted into interproton distances and entered into a distance (bounds) matrix. A distance geometry algorithm (DSPACE) was used to create embedded starting structures and to refine these structures until they showed good agreement with the distance matrix; symmetry constraints were included in the refinement procedure, making the two strands in the refined distance geometry structures virtually identical and significantly improving the agreement with the distance matrix. The NOESY spectrum for one of these distance geometry structures was then calculated from the explicit coordinates by numerically integrating all the z-magnetization transfer pathways among neighboring protons within a specified radius. Distances in this distance geometry structure that did not agree with the experimental NOESY time course were then adjusted accordingly. This process was iterated until a good agreement between calculated and experimental NOESY spectra was reached. The final structure, which generates good agreement with the experimental NOESY spectrum, displays kinks at the C3-G4 base step and at the A6-T7 base step that appear to be similar to those reported for the EcoRI restriction site DNA bound to its endonuclease. The solution structure is not the same as the crystal structure of this DNA duplex.