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.     

Structural comparison of the B-DNA dodecamers d(CGCGTTAACGCG) and d(CGCGAATTCGCG) with T2A2 and A2T2 tracts.

The x-ray structure of the deoxy oligonucleotide dodecamer d(CGCGTTAACGCG) recently determined in our laboratory shows that the helical parameters of the central TTAA segment are significantly different compared to the central AATT in d(CGCGAATTCGCG). The roll in the central TA step of the T2A2 dodecamer opens towards the minor groove while the AT step of the A2T2 dodecamer opens towards the major groove. Also, the roll angles at the steps 4 and 8 (GT and AC in T2A2) and (GA and TC in A2T2) are in opposite directions. The high cup and helical twist angles at the central base-pair of T2A2 decreases the base stacking interactions compared to A2T2. Tilt angles within the tetranucleotide segments TTAA and AATT have opposite signs. In spite of the local differences caused by the sequence inversion (TTAA----AATT), the two dodecamers exhibit similar overall bending. The top third is more bent than the bottom third relative to the central segment. This asymmetric bending in the two dodecamers is mainly due to crystal packing interactions.     

Molecular dynamics simulations of the d(CCAACGTTGG)(2) decamer: influence of the crystal environment

Molecular dynamics (MD) simulations of the DNA duplex d(CCAACGTTGG)(2) were used to study the relationship between DNA sequence and structure. Two crystal simulations were carried out; one consisted of one unit cell containing two duplexes, and the other of two unit cells containing four duplexes. Two solution simulations were also carried out, one starting from canonical B-DNA and the other starting from the crystal structure. For many helicoidal parameters, the results from the crystal and solution simulations were essentially identical. However, for other parameters, in particular, alpha, gamma, delta, (epsilon - zeta), phase, and helical twist, differences between crystal and solution simulations were apparent. Notably, during crystal simulations, values of helical twist remained comparable to those in the crystal structure, to include the sequence-dependent differences among base steps, in which values ranged from 20 degrees to 50 degrees per base step. However, in the solution simulations, not only did the average values of helical twist decrease to approximately 30 degrees per base step, but every base step was approximately 30 degrees, suggesting that the sequence-dependent information may be lost. This study reveals that MD simulations of the crystal environment complement solution simulations in validating the applicability of MD to the analysis of DNA structure.     

Structure of d(CGCGAATTCGCG) in the presence of Ca(2+) ions.

The dodecamer d(CGCGAATTCGCG) was the first oligonucleotide to be crystallized as a B-DNA duplex. Its structure was analyzed in detail in the early 1980s. Here we show that, in the presence of Ca(2+), it crystallizes in a different way (R3 space group). The dodecamers form parallel columns of straight duplexes with ten base pairs in the B form. The terminal cytosines in each molecule are disordered, whereas the terminal guanines are placed in the minor groove of neighbor duplexes. The central GAATTC region is practically identical to that found in the classic structure of the same dodecamer crystallized in the P2(1)2(1)2(1) space group in the presence of Mg(2+) and spermine. Its structure is thus independent of the crystallization conditions which have been used.     

Molecular structure of the netropsin-d(CGCGATATCGCG) complex: DNA conformation in an alternating AT segment

The molecular structure of the complex between a minor groove binding drug (netropsin) and the DNA dodecamer d(CGCGATATCGCG) has been solved and refined by single-crystal X-ray diffraction analysis to a final R factor of 20.0% to 2.4-A resolution. The crystal is similar to that of the other related dodecamers with unit cell dimensions of a = 25.48 A, b = 41.26 A, and c = 66.88 A in the space group P2(1)2(1)2(1). In the complex, netropsin binds to the central ATAT tetranucleotide segment in the narrow minor groove of the dodecamer B-DNA double helix as expected. However, in the structural refinement the drug is found to fit the electron density in two orientations equally well, suggesting the disordered model. This agrees with the results from solution studies (chemical footprinting and NMR) of the interactions between minor groove binding drugs (e.g., netropsin and distamycin A) and DNA. The stabilizing forces between drug and DNA are provided by a combination of ionic, van der Waals, and hydrogen-bonding interactions. No bifurcated hydrogen bond is found between netropsin and DNA in this complex due to the unique dispositions of the hydrogen-bond acceptors (N3 of adenine and O2 of thymine) on the floor of the DNA minor groove. Two of the four AT base pairs in the ATAT stretch have low propeller twist angles, even though the DNA has a narrow minor groove. Alternating helical twist angles are observed in the ATAT stretch with lower twist in the ApT steps than in the TpA step.     

The crystal structure analysis of d(CGCGAASSCGCG)2, a synthetic DNA dodecamer duplex containing four 4'-thio-2'-deoxythymidine nucleotides.

The crystal structure refinement of the synthetic dodecamer d(CGCGAASSCGCG), where S = 4'-thio-2'-deoxythymidine, has converged at R=0.201 for 2605 reflections with F > 2sigma(F) in the resolution range 8.0-2.4 A for a model consisting of the dodecamer duplex and 66 water molecules. A comparison of its structure with that of the native dodecamer d(CGCGAATTCGCG) has revealed that the major differences between the two structures is a change in the conformation of the sugar-phosphate backbone in the regions at and adjacent to the positions of the modified nucleosides. Examination of the fine structural parameters for each of the structures reveals that the thiosugars adopt a C3'-exo conformation in d(CGCGAASSCGCG), rather than the approximate C1'-exo conformation found for the analogous sugars in the structure of d(CGCGAATTCGCG). The observed differences in structure between the two duplexes may help to explain the enhanced resistance to nuclease digestion of synthetic oligonucleotides containing 4'-thio-2'-deoxynucleotides.     

Crystal structure of an RNA octamer duplex r(CCCIUGGG)2 incorporating tandem I.U wobbles.

The crystal structure of the RNA octamer duplex r(CCCIUGGG)2has been elucidated at 2.5 A resolution. The crystals belong to the space group P21and have unit cell constants a = 33.44 A, b = 43.41 A, c = 49.39 A and beta = 104.7 degrees with three independent duplexes (duplexes 1-3) in the asymmetric unit. The structure was solved by the molecular replacement method and refined to an Rwork/Rfree of 0.185/0.243 using 3765 reflections between 8.0 and 2.5 A. This is the first report of an RNA crystal structure incorporating I.U wobbles and three molecules in the asymmetric unit. Duplex 1 displays a kink of 24 degrees between the mismatch sites, while duplexes 2 and 3 have two kinks each of 19 degrees and 27 degrees, and 24 degrees and 29 degrees, respectively, on either side of the tandem mismatches. At the I.U/U.I mismatch steps, duplex 1 has a twist angle of 33.9 degrees, close to the average for all base pair steps, but duplexes 2 and 3 are underwound, with twist angles of 24.4 degrees and 26.5 degrees, respectively. The tandem I.U wobbles show intrastrand purine-pyrimidine stacking but exhibit interstrand purine-purine stacking with the flanking C.G pairs. The three independent duplexes are stacked non-coaxially in a head-to-tail fashion to form infinite pseudo-continuous helical columns which form intercolumn hydrogen bonding interactions through the 2'-hydroxyl groups where the minor grooves come together.     

Conformational variation of the central CG site in d(ATGACGTCAT)2 and d(GAAAACGTTTTC)2. An NMR, molecular modelling and 3D-homology investigation.

The determination of the solution structure of two self-complementary oligomers d(ATGACGTCAT)2 (CG10) and d(GAAAACGTTTTC)2 (CG12), both containing the 5'-pur-ACGT-pyr-3' sequence, is reported. The impact of the base context on the conformation of the central CpG site has been examined by a combined approach of: (a) 2D 1H-NMR and 31P-NMR; (b) molecular mechanics under experimental constraints; (c) back-calculations of NOESY spectra and iterative refinements of distances; and (d) 3D-homology search of the central tetrad ACGT within the complete oligonucleotides. A full NMR study of each fragment is achieved by means of standard 2D experiments: NOESY, 2D homonuclear Hartmann-Hahn spectroscopy, double-quantum-filtered COSY and heteronuclear 1H-31P correlation. Sugar phase angle, epsilon-zeta difference angle and NOE-derived distances are input as experimental constraints to generate molecular models by energy minimization with the help of jumna. The morass program is used to iteratively refine the structures obtained. The similarity of the two ACGTs within the whole oligonucleotides is investigated. Both the decamer and the dodecamer adopt a B-like DNA conformation. However, the helical parameters within this conformational type are significantly different in CG12 and CG10. The central CpG step conformation is not locked by its nearest environment (5'A and 3'T) as seen from the structural analysis of ACGT in the two molecules. In CG12, despite the presence of runs of A-T pairs, CpG presents a high twist of 43 degrees and a sugar phase at the guanine of about 180 degrees, previously observed in other ACGT-containing-oligomers. Conversely, ACGT in CG10 exhibits strong inclinations, positive rolls, a flat profile of sugar phase, twist and glycosidic angles, as a result of the nucleotide sequence extending beyond the tetrad. The structural specificity of CG10 and its flexibility (as reflected by its energy) are tentatively related to the process of recognition of the cyclic AMP response element by its cognate protein.     

Unusual intercalation of acridin-9-ylthiourea into the 5'-GA/TC DNA base step from the minor groove: implications for the covalent DNA adduct profile of a novel platinum-intercalator conjugate

The binding of the novel cytotoxic acridine derivative, 1-[2-(acridin-9-ylamino)ethyl]-1,3-dimethylthiourea (ACRAMTU) to various self-complementary oligonucleotide duplexes has been studied by combined high-resolution NMR spectroscopy/restrained molecular dynamics and equilibrium binding assays to establish the sequence and groove specificity of intercalation. The binding mode in the sequences d(GGACGTCC)₂ and d(GGAGCTCC)₂ was deduced from chemical shift changes and intermolecular NOEs between the ligand and the oligonucleotides. ACRAMTU intercalated into the 5′-CG/CG and 5′-GA/TC base steps, and penetration of the duplexes occurred from the minor groove. Intercalation of ACRAMTU in d(GGTACC)₂ occurs at the central TA/TA step, based on the absence of the internucleotide A4H8–T3H1′ and A4H8–T3H3′ cross-peaks in the 1:1 complex of this sequence. An energy- minimized AMBER model of the 1:2 complex, [d(GGAGCTCC)₂(ACRAMTU)₂], was generated, which was based on restricted molecular dynamics/ mechanics calculations using 108 NOE distance restraints (including 11 DNA–drug distances per ligand). Equilibrium dialysis experiments were performed using octamers containing various base steps present in the ‘NMR sequences’. The highest affinity for ACRAMTU was observed in d(TATAT ATA)₂, followed by d(CGCGCGCG)₂ and d(GAG ATCTC)₂. The binding levels for CG/CG and GA/TC were virtually the same. The unusual tolerance of the GA/TC intercalation site and the pronounced groove specificity of ACRAMTU play a significant role in the molecular recognition between the corresponding platinum conjugate, Pt-ACRAMTU, and DNA.     

Binding of a Hoechst dye to d(CGCGATATCGCG) and its influence on the conformation of the DNA fragment

Hoechst dye 33258 is a planar drug molecule that binds to the minor groove of DNA, especially where there are a number of A.T base pairs. We have solved the structure of the Hoechst dye bound to the DNA dodecamer d(CGCGATATCGCG) at 2.3 A. This structure is compared to that of the same dodecamer with the minor-groove-binding drug netropsin bound to it, as well as to structures that have been solved for this Hoechst dye bound to a DNA dodecamer containing the central four base pairs with the sequence AATT. We find that the position of the Hoechst drug in this dodecamer is quite different from that found in the other dodecamer since it has an opposite orientation compared to the other two structures. The drug covers three of the four A.T base pairs and extends its piperazine ring to the first G.C base pair adjacent to the alternating AT segment. Furthermore, the drug binding has modified the structure of the DNA dodecamer. Other DNA dodecamers with alternating AT sequences show an alternation in the size of the helical twist between the ApT step (small twist) and the TpA step (large twist). In this structure the alternation is reversed with larger twists in the ApT steps than in the TpA step. In addition, there is a rotation of one of the thymine bases in the DNA dodecamer that is associated with hydrogen bonding to the Hoechst drug. This structure illustrates the considerable plasticity found in the DNA molecule when it binds to different planar molecules inserted into the minor groove.     

Design of phosphoramidite monomer for optimal incorporation of functional intercalator to main chain of oligonucleotide

Chirally pure phosphoramidite monomers bearing 9-amino-6-chloro-2-methoxyacridine were synthesized from D- or L-threoninol and omega-aminocarboxylic acid, and incorporated into oligonucleotides. These acridine-DNA conjugates formed stable duplexes with complementary RNA because of intercalation of the acridine to DNA/RNA heteroduplexes. The stability of duplexes was not very dependent on either the chirality of the central carbon bearing the acridine or the length of the side chain. However, the ability for site-selective activation of the phosphodiester linkage in front of the acridine, which induced Lu(III)-promoted RNA scission, was strongly dependent on these two factors. The largest activation was achieved when the monomer unit was prepared from L-threoninol and 4-aminobutyric acid and the acridine was bound to the amino group. By attaching the more acidic 9-amino-2-methoxy-6-nitroacridine to this optimized scaffold, a quite effective acridine-DNA conjugate for site-selective RNA scission was obtained.     

X-Ray analysis of d(CGCGAATTXGCG)(2) containing a 2' or minute-deoxy-N(4)-methoxycytosine residue at X: a characteristic pattern of sugar puckers in the crystalline state of the Dickerson-Drew type DNA dodecamers

In a series of structural studies on damaged DNA, a modified Dickerson-Drew dodecamer with the sequence d(CGCGAATTmo(4)CGCG), where mo(4)C is 2'-deoxy-N(4)-methoxycytidine, was synthesized and its structure in a new crystal form has been determined by the X-ray diffraction method. The two dodecamers form a B-form duplex, in which the two mo(4)C residues, respectively, form a wobble pair and a Watson-Crick type pair with the guanine residues of the opposite strand. A comparison of the sugar conformations with those of the other related Dickerson-Drew dodecamers indicates a common feature of their puckering patterns. The sugar pucker of the third residue always adopts an intermediate state (C4'-exo-O4'-endo) between the A-form and B-form. This deviation is ascribed to the stacking interaction of the ribose ring at the third residue with the guanine base at the 12th residue, which is brought about by an extra G12:G2 interaction between two duplexes related by a crystallographic 2(1) symmetry.     

Crystal structure of the topoisomerase II poison 9-amino-[N-(2-dimethylamino)ethyl]acridine-4-carboxamide bound to the DNA hexanucleotide d(CGTACG)2.

The structure of the complex formed between d(CGTACG)(2) and the antitumor agent 9-amino-[N-(2-dimethylamino)ethyl]acridine-4-carboxamide has been solved to a resolution of 1.6 A using X-ray crystallography. The complex crystallized in space group P6(4) with unit cell dimensions a = b = 30.2 A and c = 39.7 A, alpha = beta = 90 degrees, gamma = 120 degrees. The asymmetric unit contains a single strand of DNA, 1. 5 drug molecules, and 29 water molecules. The final structure has an overall R factor of 19.3%. A drug molecule intercalates between each of the CpG dinucleotide steps with its side chain lying in the major groove, and the protonated dimethylamino group partially occupies positions close to ( approximately 3.0 A) the N7 and O6 atoms of guanine G2. A water molecule forms bridging hydrogen bonds between the 4-carboxamide NH and the phosphate group of the same guanine. Sugar rings adopt the C2'-endo conformation except for cytosine C1 which moves to C3'-endo, thereby preventing steric collision between its C2' methylene group and the intercalated acridine ring. The intercalation cavity is opened by rotations of the main chain torsion angles alpha and gamma at guanines G2 and G6. Intercalation perturbs helix winding throughout the hexanucleotide compared to B-DNA, steps 1 and 2 being unwound by 8 degrees and 12 degrees, respectively, whereas the central TpA step is overwound by 17 degrees. An additional drug molecule, lying with the 2-fold axis in the plane of the acridine ring, is located at the end of each DNA helix, linking it to the next duplex to form a continuously stacked structure. The protonated N,N-dimethylamino group of this "end-stacked" drug hydrogen bonds to the N7 atom of guanine G6. In both drug molecules, the 4-carboxamide group is internally hydrogen bonded to the protonated N-10 atom of the acridine ring. The structure of the intercalated complex enables a rationalization of the known structure-activity relationships for inhibition of topoisomerase II activity, cytotoxicity, and DNA-binding kinetics for 9-aminoacridine-4-carboxamides.     

Alternation of DNA and Solvent Layers in the A Form of d(GGCGCC) Obtainhted by Ethanol Crystallization

Abstract

We have determined by X-ray crystallography the structure of the hexamer duplex d(GGCGCC)₂ in the A-form using ethanol as a precipitant. The same sequence had previously been crystallized in the B-form, but with 2-methyl-2, 4-pentanediol as a precipitant. It appears that ethanol precipitation is a useful method to induce the formation of A-form crystals of DNA. Packing of the molecules in the crystal has unique features: the known interaction of A-DNA duplexes between terminal base-pairs and the minor groove of neighbor molecules is combined with a superstructure consisting in an alternation of DNA layers and solvent layers (water/ions). This organization in layers has been observed before, also with hexamers in the A conformation which crystallize in the same space group (C222 ₁). The solvent layer has a precise thickness, although very few ordered water molecules can be detected. Another feature of this crystal is its large unit cell, which gives rise to an asymmetric unit with three hexamer duplexes. One of the three duplexes is quite different from the other two in several aspects: the number of base pairs per turn, the twist pattern, the mean value of the twist angle and the fact that one terminal base-pair is not stacked as part of the duplex and appears to be disordered. So the variability in conformation of this sequence is remarkable.     

Alternation of DNA and solvent layers in the A form of d(GGCGCC) obtained by ethanol crystallization

We have determined by X-ray crystallography the structure of the hexamer duplex d(GGCGCC)2 in the A-form using ethanol as a precipitant. The same sequence had previously been crystallized in the B-form, but with 2-methyl-2,4-pentanediol as a precipitant. It appears that ethanol precipitation is a useful method to induce the formation of A-form crystals of DNA. Packing of the molecules in the crystal has unique features: the known interaction of A-DNA duplexes between terminal base-pairs and the minor groove of neighbor molecules is combined with a superstructure consisting in an alternation of DNA layers and solvent layers (water/ions). This organization in layers has been observed before, also with hexamers in the A conformation which crystallize in the same space group (C2221). The solvent layer has a precise thickness, although very few ordered water molecules can be detected. Another feature of this crystal is its large unit cell, which gives rise to an asymmetric unit with three hexamer duplexes. One of the three duplexes is quite different from the other two in several aspects: the number of base pairs per turn, the twist pattern, the mean value of the twist angle and the fact that one terminal base-pair is not stacked as part of the duplex and appears to be disordered. So the variability in conformation of this sequence is remarkable.     

A novel form of intercalation involving four DNA duplexes in an acridine-4-carboxamide complex of d(CGTACG)(2)

The structures of the complexes formed between 9-amino-[N-(2-dimethyl-amino)butyl]acridine-4-carboxamide and d(CG^5BrUACG)₂ and d(CGTACG)₂ have been solved by X-ray crystallography using MAD phasing methodology and refined to a resolution of 1.6 Å. The complexes crystallised in space group C222. An asymmetric unit in the brominated complex comprises two strands of DNA, one disordered drug molecule, two cobalt (II) ions and 19 water molecules (31 in the native complex). Asymmetric units in the native complex also contain a sodium ion. The structures exhibit novel features not previously observed in crystals of DNA/drug complexes. The DNA helices stack in continuous columns with their central 4 bp adopting a B-like motif. However, despite being a palindromic sequence, the terminal GC base pairs engage in quite different interactions. At one end of the duplex there is a CpG dinucleotide overlap modified by ligand intercalation and terminal cytosine exchange between symmetry-related duplexes. A novel intercalation complex is formed involving four DNA duplexes, four ligand molecules and two pairs of base tetrads. The other end of the DNA is frayed with the terminal guanine lying in the minor groove of the next duplex in the column. The structure is stabilised by guanine N7/cobalt (II) coordination. We discuss our findings with respect to the effects of packing forces on DNA crystal structure, and the potential effects of intercalating agents on biochemical processes involving DNA quadruplexes and strand exchanges. NDB accession numbers: DD0032 (brominated) and DD0033 (native).     

Oxetane locked thymidine in the Dickerson-Drew dodecamer causes local base pairing distortions -- an NMR structure and hydration study

The introduction of a North-type sugar conformation constrained oxetane T block, 1-(1',3'-O-anhydro-beta-D-psicofuranosyl) thymine, at the T(7) position of the self-complementary Dickerson-Drew dodecamer, d[(5'-C(1)G(2)C(3)G(4)A(5)A(6)T(7)T(8)C(9)G(10)C(11)G(12)-3')](2), considerably perturbs the conformation of the four central base pairs, reducing the stability of the structure. UV spectroscopy and 1D NMR display a drop in melting temperature of approximately 10 degrees C per modification for the T(7) oxetane modified duplex, where the T(7) block has been introduced in both strands, compared to the native Dickerson-Drew dodecamer. The three dimensional structure has been determined by NMR spectroscopy and has subsequently been compared with the results of 2.4 ns MD simulations of the native and the T(7) oxetane modified duplexes. The modified T(7) residue is found to maintain its constrained sugar- and the related glycosyl torsion conformations in the duplex, resulting in staggered and stretched T(7).A(6) and A(6).T(7) non-linear base pairs. The stacking is less perturbed, but there is an increased roll between the two central residues compared to the native counterpart, which is compensated by tilts of the neighboring base steps. The one dimensional melting profile of base protons of the T(7) and T(8) residues reveals that the introduction of the North-type sugar constrained thymine destabilizes the core of the modified duplex, promoting melting to start simultaneously from the center as well as from the ends. Temperature dependent hydration studies by NMR demonstrate that the central T(7).A(6)/A(6).T(7) base pairs of the T(7) oxetane modified Dickerson-Drew dodecamer have at least one order of magnitude higher water exchange rates (correlated to the opening rate of the base pair) than the corresponding base pairs in the native duplex.     

Crystal structure of the B-DNA hexamer d(CTCGAG): model for an A-to-B transition.

The crystal structure of the B-DNA hexamer d(CTCGAG) has been solved at 1.9 A resolution by iterative single isomorphous replacement, using the brominated derivative d(CG5BrCGAG), and refined to an R-factor of 18.6% for 120 nonhydrogen nucleic acid atoms and 32 water molecules. Although the central four base pairs form a typical B-form helix, several parameters suggest a transition to an A-like conformation at the termini. Based on this observation, a B-to-A transition was modeled, maintaining efficient base stacking across the junction. The wide minor groove (approximately 6.9 A) is reminiscent of that in the side-by-side double drug-DNA complexes and hosts a double spine of hydration. The global helix axes of the pseudo-continuous helices are at an acute angle of 60 degrees. The pseudocontinuous stacking is reinforced by the minor groove water structure extending between the two duplexes. The crossover point of two pairs of stacked duplexes is at the stacking junction, unlike that observed in the B-DNA decamers and dodecamers. This arrangement may have implications for the structure of a four-way DNA junction. The duplexes are arranged around a large (approximately 20 A diameter) channel centered on a 6(2) screw axis.     

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.     

Synthesis of twisted intercalating nucleic acids possessing acridine derivatives. Thermal stability studies

Twisted intercalating nucleic acids (TINA) possessing acridine derivatives have been synthesized via the postsynthetic modifications of oligonucleotides possessing insertions of (R)-1-O-(4-iodobenzyl)glycerol (8) or (R)-1-O-(4-ethynylbenzyl)glycerol (9) at the 5'-end or in the middle as a bulge. In the first postsynthetic step, oligonucleotides 8 and 9 on the CPG support were treated with a Sonogashira coupling reaction mixture containing 9-chloro-2-ethynylacridine or 9-chloro-2-iodoacridine, respectively. After the postsynthetic step, treatment of the oligonucleotides with 32% aq ammonia or 50% ethanolic solution of tris(2-aminoethyl)amine led to the substitution of chloride on acridine concurrent with deprotection of the bases and cleavage of the oligonucleotides from CPG. Molecular modeling of the parallel triplex with a bulged insertion of the monomer (R)-3-O-[4-(9-aminoacridin-2-ylethynyl)benzyl]glycerol in the triplex-forming oligonucleotide (TFO) showed that the acridine moiety was stacking between the bases of the duplex, while phenyl was placed between the bases of the TFO. Thermal denaturation studies and fluorescence properties of TINA-acridine oligonucleotide duplexes and triplexes are discussed.