Interactions between an anthracycline antibiotic and DNA: molecular structure of daunomycin complexed to d(CpGpTpApCpG) at 1.2-A resolution

The crystal structure of a daunomycin-d(CGTACG) complex has been solved by X-ray diffraction analysis and refined to a final R factor of 0.175 at 1.2-A resolution. The crystals are in a tetragonal crystal system with space group P4(1)2(1)2 and cell dimensions of a = b = 27.86 A and c = 52.72 A. The self-complementary DNA forms a six base pair right-handed double helix with two daunomycin molecules intercalated in the d(CpG) sequences at either end of the helix. Daunomycin in the complex has a conformation different from that of daunomycin alone. The daunomycin aglycon chromophore is oriented at right angles to the long dimension of the DNA base pairs, and the cyclohexene ring A rests in the minor groove of the double helix. Substituents on this ring have hydrogen-bonding interactions to the base pairs above and below the intercalation site. O9 hydroxyl group of the daunomycin forms two hydrogen bonds with N3 and N2 of an adjacent guanine base. Two bridging water molecules between the drug and DNA stabilize the complex in the minor groove. In the major groove, a hydrated sodium ion is coordinated to N7 of the terminal guanine and the O4 and O5 of daunomycin with a distorted octahedral geometry. The amino sugar lies in the minor groove without bonding to the DNA. The DNA double helix is distorted with an asymmetrical rearrangement of the backbone conformation surrounding the intercalator drug. The sugar puckers are C1,C2'-endo, G2,C1'-endo, C11,C1'-endo, and G12,C3'-exo. Only the C1 residue has a normal anti-glycosyl torsion angle (chi = -154 degrees), while the other three residues are all in the high anti range (average chi = -86 degrees). This structure allows us to identify three principal functional components of anthracycline antibiotics: the intercalator (rings B-D), the anchoring functions associated with ring A, and the amino sugar. The structure-function relationships of daunomycin binding to DNA as well as other related anticancer drugs are discussed.     

Solution structure of a five-adenine bulge loop within a DNA duplex.

The three-dimensional solution structure of a DNA molecule of the sequence 5'-d(GCATCGAAAAAGCTACG)-3' paired with 5'-d(CGTAGCCGATGC)-3' containing a five-adenine bulge loop (dA(5)-bulge) between two double helical stems was determined by 2D (1)H and (31)P NMR, infrared, and Raman spectroscopy. The DNA in both stems adopt a classical B-form double helical structure with Watson-Crick base pairing and C2'-endo sugar conformation. In addition, the two dG/dC base pairs framing the dA(5)-bulge loop are formed and are stable at least up to 30 degrees C. The five adenine bases of the bulge loop are localized at intrahelical positions within the double helical stems. Stacking on the double helical stem is continued for the first four 5'-adenines in the bulge loop. The total rise (the height) of these four stacked adenines roughly equals the diameter of the double helical stem. The stacking interactions are broken between the last of these four 5'-adenines and the fifth loop adenine at the 3'-end. This 3'-adenine partially stacks on the other stem. The angle between the base planes of the two nonstacking adenines (A10 and A11) in the bulge loop reflects the kinking angle of the global DNA structure. The neighboring cytosines opposite the dA(5)-bulge (being parts of the bulge flanking base pairs) do not stack on one another. This disruption of stacking is characterized by a partial shearing of these bases, such that certain sequential NOEs for this base step are preserved. In the base step opposite the loop, an extraordinary hydrogen bond is observed between the phosphate backbone of the 5'-dC and the amino proton of the 3'-dC in about two-thirds of the conformers. This hydrogen bond probably contributes to stabilizing the global DNA structure. The dA(5)-bulge induces a local kink into the DNA molecule of about 73 degrees (+/-11 degrees ). This kinking angle and the mutual orientation of the two double helical stems agree well with results from fluorescence resonance energy transfer measurements of single- and double-bulge DNA molecules.     

Binding of a macrocyclic bisacridine and ametantrone to CGTACG involves similar unusual intercalation platforms

The binding of a macrocyclic bisacridine and an antitumor intercalator ametantrone to DNA has been studied. We carried out X-ray diffraction analyses of the complexes between both intercalators and CGTACG. We have determined the crystal structure, by the multiple-wavelength anomalous diffraction (MAD) method, of bisacridine complexed with CGTA[br(5)C]G at 1.8 A resolution. The refined native crystal structure at 1.1 A resolution (space group C222, a = 29.58 A, b = 54.04 A, c = 40.22 A, and R-factor = 0.163) revealed that only one acridine of the bisacridine drug binds at the C5pG6 step of the DNA, with the other acridine plus both linkers completely disordered. Surprisingly, both terminal G.C base pairs are unraveled. The C1 nucleotide is disordered, and the G2 base is bridged to its own phosphate P2 through a hydrated Co(2+) ion. G12 is swung toward the minor groove with its base stacked over the backbone. The C7 nucleotide is flipped away from the duplex part and base paired to a 2-fold symmetry-related G6. The central four base pairs adopt the B-DNA conformation. An unusual intercalator platform is formed by bringing four complexes together (involving the 222 symmetry) such that the intercalator cavity is flanked by two sets of G x C base pairs (i.e., C5 x G8 and G6 x C7) on each side, joined together by G6 x G8 tertiary base pairing interactions. In the bisacridine-CGTACG complex, the intercalation platform is intercalated with two acridines, whereas in the ametantrone-CGTACG complex, only one ametantrone is bound. NMR titration of the bisacridine to AACGATCGTT suggests that the bisacridine prefers to bridge more than one DNA duplex by intercalating each acridine to different duplexes. The results may be relevant in understanding binding of certain intercalators to DNA structure associated with the quadruplet helix and Holliday junction.     

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.     

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.     

A molecular mechanical study of complexes formed between 4-nitroquinoline-N-oxide and dinucleoside phosphates.

Molecular mechanical calculations were done on complexes of 4-nitroquinoline-N-oxide (NQO) with various dinucleoside phosphates [(ApT)2, (CpG)2, (GpC)2, and (TpA)2]. Models built using proflavine (uniform C3' endo sugar puckers) and acridine orange (mixed C3' endo (3'-5') C2' endo sugar puckers) dinucleoside phosphate X-ray structures were used in the calculations. Relative binding energies, complex geometries, and various intercalator orientations in the complexes were studied. The results suggest qualitatively different geometries for pyr-(3'-5')-pur and pur-(3'-5')-pyr sequences. Specifically, we find marked distortion in some of the complexes (i.e. there is not a parallel coplanar relationship between the base pairs and intercalator), distortion of the NQO nitro group from planarity in the complexes and mobility of NQO in the intercalation site. We suggest that experimental studies of NQO-dinucleoside phosphate complexes may reveal intercalation complexes which deviate substantially more from a nearly parallel coplanar arrangement of bases and intercalator than has been previously observed.     

Self base pairing in a complementary deoxydinucleoside monophosphate duplex: crystal and molecular structure of deoxycytidylyl-(3'-5')-deoxyguanosine

The molecular structure of ammonium deoxycytidylyl-(3'-5')-deoxyguanosine, crystallized from aqueous acetone near pH 4, was determined for X-ray diffraction data. The crystals were tetragonal, space group P43212 with a = b = 11.078 (1) A and c = 45.826 (4) A. The structure was solved by tangent expansion of phases based on a derived phosphorus position and refined to R = 0.060 by full matrix least squares. Molecules related by a 2-fold symmetry axis are connected by hydrogen bonds between the bases and form parallel right-handed duplexes. Pairs of cytosines share a proton at N(3) and are joined by three hydrogen bonds: N(4)-H...O(2)...H-N(4), and N(3)-H...N(3). Guanines are joined by two hydrogen bonds: N(2)-H...N(3) and N(3)...H-N(2). Base-stacking interactions within the duplex are weak with the cytosine and guanine ring planes inclined at 24 degrees to each other in each monomer. Despite the unusual arrangement of the molecules, the sugar phosphate backbone has the g-g- conformation normally associated with right-handed double helical structures. Conformational parameters of the nucleosides are also typical with both sugars C(2')-endo and glycosidic torsion angles 55 degrees for cytidine and 94 degrees for guanosine. The bonding geometry of the bases is influenced by hydrogen bonding and charge-transfer networks in the crystal lattice. The solvent molecules interact with the dimer in three fused circular hydrogen bonding domains with a single disordered ammonium cation per d(CpG) dimer. Parallels with the formation of self base pairs and their implications in molecular biology are discussed.     

G.T wobble base-pairing in Z-DNA at 1.0 A atomic resolution: the crystal structure of d(CGCGTG).

The DNA oligomer d(CGCGTG) crystallizes as a Z-DNA double helix containing two guanine-thymine base pair mismatches of the wobble type. The crystal diffracts to 1 A resolution and the structure has been solved and refined. At this resolution, a large amount of information is revealed about the organization of the water molecules in the lattice generally and more specifically around the wobble base pairs. By comparing this structure with the analogous high resolution structure of d(CGCGCG) we can visualize the structural changes as well as the reorganization of the solvent molecules associated with wobble base pairing. There is only a small distortion of the Z-DNA backbone resulting from introduction of the GT mismatched base pairs. The water molecules cluster around the wobble base pair taking up all of the hydrogen bonding capabilities of the bases due to wobble pairing. These bridging water molecules serve to stabilize the base-base interaction and, thus, may be generally important for base mispairing either in DNA or in RNA molecules.     

Recognition of hairpin-containing single-stranded DNA by oligonucleotides containing internal acridine derivatives.

Oligodeoxynucleotides with an internal intercalating agent have been targeted to single-stranded sequences containing hairpin structures. The oligonucleotide binds to nonadjacent single-stranded sequences on both sides of the hairpin structure in such a way as to form a three-way junction. The acridine derivative is inserted at a position that allows it to interact with the three-way junction. The melting temperature (Tm) of complexes formed between the hairpin-containing target and oligonucleotides containing one internal acridine derivative was higher than that obtained with the same target and an unmodified oligonucleotide (DeltaTm = +13 degrees C). The internal acridine provided the oligonucleotide with a higher affinity than covalent attachment to the 5' end. Oligonucleotides could also be designed to recognize a hairpin-containing single-stranded nucleic acid by formation of Watson-Crick hydrogen bonds with a single-stranded part and Hoogsteen hydrogen bonds with the stem of the hairpin. An internal acridine derivative was introduced at the junction between the two domains, the double helix domain with Watson-Crick base pairs and the triple helix domain involving Hoogsteen base triplets in the major groove of the hairpin stem. Oligonucleotides with an internal acridine or an acridine at their 5' end have similar binding affinities for the stem-loop-containing target. The bis-modified oligonucleotide containing two acridines, one at the 5' end and one at an internal site, did not exhibit a higher affinity than the oligonucleotides with only one intercalating agent. The design of oligonucleotides with an internal intercalating agent might be of interest to control gene expression through recognition of secondary structures in single-stranded targets.     

Conformation and dynamics of drug-DNA intercalation.

Molecular dynamics simulations have been undertaken for a B-form dodecanucleotide duplex in solution with and without an intercalated proflavine molecule between the central C.G base pairs. The introduction of this simple intercalator affects both the conformational features and dynamic properties of the oligonucleotide double helix. Changes are seen in the rms atomic fluctuations and anisotropy of phosphate, sugar and base atoms. The backbone conformation is slightly changed on average and more sugars adopt the C3' endo conformation in the simulation of the complex compared with the simulation of the oligonucleotide alone. Both major and minor grooves becomes wider on average with the addition of the intercalating drug. Flanking A.T base pairs on both sides of the intercalation site have undergone an increase in flexibility, with the base pairs, especially at the 5' side, having the N1...N3 hydrogen bonds being broken.     

AT base pairs are less stable than GC base pairs in Z-DNA: The crystal structure of d(m5CGTAm5CG)

Two hexanucleoside pentaphosphates, 5-methyl and 5-bromo cytosine derivatives of d(CpGpTp-ApCpG) have been synthesized, crystallized, and their three-dimensional structure solved. They both form left-handed Z-DNA and the methylated derivative has been refined to 1.2 Å resolution. These are the first crystal Z-DNA structures that contain AT base pairs. The overall form of the molecule is very similar to that of the unmethylated or the fully methylated (dC-dG)₃ hexamer although there are slight changes in base stacking. However, significant differences are found in the hydration of the helical groove. When GC base pairs are present, the helical groove is systematically filled with two water molecules per base pair hydrogen bonded to the bases. Both of these water molecules are not seen in the electron density map in the segments of the helix containing AT base pairs, probably because of solvent disorder. This could be one of the features that makes AT base pairs form Z-DNA less readily than GC base pairs.     

Hydrogen and hydration of DNA and RNA oligonucleotides

In this paper, hydrogen bonding interaction and hydration in crystal structures of both DNA and RNA oligonucleotides are discussed. Their roles in the formation and stabilization of oligonucleotides have been covered. Details of the Watson-Crick base pairs G.C and A.U in DNA and RNA are illustrated. The geometry of the wobble (mismatched) G.U base pairs and the cis and almost trans conformations of the mismatched U.U base pairs in RNA is described. The difference in hydration of the Watson-Crick base pairs G.C, A.U and the wobble G.U in different sequences of codon-anticodon interaction in double helical molecules are indicative of the effect of hydration. The hydration patterns of the phosphate, the 2'-hydroxyl groups, the water bridges linking the phosphate group, N7 (purine) and N4 of Cs or O4 of Us in the major groove, the water bridges between the 2'-hydroxyl group and N3 (purine) and O2 (pyrimidine) in the minor groove are discussed.     

Mediation of the A/B-DNA helix transition by G-tracts in the crystal structure of duplex CATGGGCCCATG

The crystal structure of the DNA dodecamer duplex CATGGGCCCATG lies on a structural continuum along the transition between A- and B-DNA. The dodecamer possesses the normal vector plot and inclination values typical of B-DNA, but has the crystal packing, helical twist, groove width, sugar pucker, slide and x-displacement values typical of A-DNA. The structure shows highly ordered water structures, such as a double spine of water molecules against each side of the major groove, stabilizing the GC base pairs in an A-like conformation. The different hydration of GC and AT base pairs provides a physical basis for solvent-dependent facilitation of the A↔B helix transition by GC base pairs. Crystal structures of CATGGGCCCATG and other A/B-DNA intermediates support a ‘slide first, roll later’ mechanism for the B→A helix transition. In the distribution of helical parameters in protein–DNA crystal structures, GpG base steps show A-like properties, reflecting their innate predisposition for the A conformation.     

Cyclic diguanylic acid behaves as a host molecule for planar intercalators

Cyclic ribodiguanylic acid, c-(GpGp), is the endogenous effector regulator of cellulose synthase. Its three-dimensional structure from two different crystal forms (tetragonal and trigonal) has been determined by X-ray diffraction analysis at 1 A resolution. In both crystal forms, two independent c-(GpGp) molecules associate with each other to form a self-intercalated dimer. A hydrated cobalt ion is found to coordinate to two N7 atoms of adjacent guanines, forcing these two guanines to destack with a large dihedral angle (32 degrees), in the dimer of the tetragonal form. This metal coordination mechanism may be relevant to that of the anticancer drug cisplatin. Moreover, c-(GpGp) exhibits unusual spectral properties not seen in any other cyclic dinucleotide. It interacts with planar organic intercalator molecules in ways similar to double helical DNA. We propose a cage-like model consisting of a tetrameric c-(GpGp) aggregate in which a large cavity ('host') is generated to afford a binding site for certain planar intercalators ('guests').     

DNA Intercalation and Photoinduced Cleavage by 4-Nitro(N-Hexylamine)1,8-Naphthalimide

Abstract

A novel intercalator, 4-nitro(N-hexylamine)1,8-naphthalimide, was synthesised and its DNA binding and photoinduced DNA cleavage properties were studied. The DNA unwinding results show that it binds through intercalation. Absorption and fluorescence spectroscopy reveal the preference for A/T base pairs as compared to G/C base pairs for the binding. The intercalator produces photoinduced single strand scissions in double helical DNA.     

Visualisation of a 2'-5' parallel stranded double helix at atomic resolution: crystal structure of cytidylyl-2',5'-adenosine

X-ray crystallographic studies on 3'-5' oligomers have provided a great deal of information on the stereochemistry and conformational flexibility of nucleic acids and polynucleotides. In contrast, there is very little information available on 2'-5' polynucleotides. We have now obtained the crystal structure of Cytidylyl-2',5'-Adenosine (C2'p5'A) at atomic resolution to establish the conformational differences between these two classes of polymers. The dinucleoside phosphate crystallises in the monoclinic space group C2, with a = 33.912(4)A, b = 16.824(4)A, c = 12.898(2)A and beta = 112.35(1) with two molecules in the asymmetric unit. Spectacularly, the two independent C2'p5'A molecules in the asymmetric unit form right handed miniature parallel stranded double helices with their respective crystallographic two fold (b axis) symmetry mates. Remarkably, the two mini duplexes are almost indistinguishable. The cytosines and adenines form self-pairs with three and two hydrogen bonds respectively. The conformation of the C and A residues about the glycosyl bond is anti same as in the 3'-5' analog but contrasts the anti and syn geometry of C and A residues in A2'p5'C. The furanose ring conformation is C3' endo, C2' endo mixed puckering as in the C3'p5'A-proflavine complex. A comparison of the backbone torsion angles with other 2'-5' dinucleoside structures reveals that the major deviations occur in the torsion angles about the C3'-C2' and C4'-C3' bonds. A right-handed 2'-5' parallel stranded double helix having eight base pairs per turn and 45 degrees turn angle between them has been constructed using this dinucleoside phosphate as repeat unit. A discussion on 2'-5' parallel stranded double helix and its relevance to biological systems is presented.     

Interaction of nucleic acid bases with water molecules and formation of mismatched nucleotide pairs

The possibility of the inclusion of water molecules in the formation of mismatched nucleotide pairs was considered in relation to the mechanisms of point errors in template directed biosynthesis. Calculations of the intermolecular interaction energy for systems containing two bases and one water molecule were carried out by the method of atom-atom potential functions. There exist energy minima for each base pair, corresponding to a single N--H...O or N--H...N H-bond between the bases and H-bonding of the water molecule with both bases. The relative positions of glycosyl bonds in some of these minima are closer to those for Watson--Crick pairs, than the positions of minima for these pairs without water. For other minima, the H-bond formation between the water molecule and the two bases additionally stabilizes the relative base position in wobble-pairs with two H-bonds between the bases. The base and water positions in energy minima are compared with the positions in some pairs proposed on the basis of NMR and X-ray data for double helical oligonucleotides.     

Secondary structure of nuclear precursors of the informational RNA (pre-mRNA)]

The secondary structure of pre-mRNA species from mouse Ehrlich ascites carcinoma cells extracted with phenol at the temperatures either 55-65 degrees C or 65-85 degrees C was investigated. A fraction of the double helical regions of pre-mRNA was estimated by two methods: a) by recording of melting curves; b) by measuring fluorescence lifetimes of acridine orange dye adsorbed on the nucleic acid. This fraction was about 64-68%. Further lowering of ionic strength down to 0.024 results in 10-15% decrease in the fraction of double regions. Both lowering of ionic strength and increase of the temperature up to 50-55 degrees C results in despiralisation of pre-mRNA regions which contain more than 70% of AU-nucleotide pairs. Only regions containing mainly GC-nucleotide pairs remain double-stranded under heating to temperatures above 50 degrees C. These facts were established on the basis of studies of acriflavin dye complexes with pre-mRNA.     

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.