The structure of guanosine-thymidine mismatches in B-DNA at 2.5-A resolution

The structure of the deoxyoligomer d(C-G-C-G-A-A-T-T-T-G-C-G) was determined at 2.5-A resolution by single crystal x-ray diffraction techniques. The final R factor is 18% with the location of 71 water molecules. The oligomer crystallizes in a B-DNA-type conformation, with two strands interacting to form a dodecamer duplex. The double helix consists of four A X T and six G X C Watson-Crick base pairs and two G X T mismatches. The G X T pairs adopt a "wobble" structure with the thymine projecting into the major groove and the guanine into the minor groove. The mispairs are accommodated in the normal double helix by small adjustments in the conformation of the sugar phosphate backbone. A comparison with the isomorphous parent compound containing only Watson-Crick base pairs shows that any changes in the structure induced by the presence of G X T mispairs are highly localized. The global conformation of the duplex is conserved. The G X T mismatch has already been studied by x-ray techniques in A and Z helices where similar results were found. The geometry of the mispair is essentially identical in all structures so far examined, irrespective of the DNA conformation. The hydration is also similar with solvent molecules bridging the functional groups of the bases via hydrogen bonds. Hydration may be an important factor in stabilizing G X T mismatches. A characteristic of Watson-Crick paired A X T and G X C bases is the pseudo 2-fold symmetry axis in the plane of the base pairs. The G X T wobble base pair is pronouncedly asymmetric. This asymmetry, coupled with the disposition of functional groups in the major and minor grooves, provides a number of features which may contribute to the recognition of the mismatch by repair enzymes.     

Interactions of quinoxaline antibiotic and DNA: the molecular structure of a triostin A-d(GCGTACGC) complex

The crystal structure of a DNA octamer d(GCGTACGC) complexed to an antitumor antibiotic, triostin A, has been solved and refined to 2.2 A resolution by x-ray diffraction analysis. The antibiotic molecule acts as a true bis intercalator surrounding the d(CpG) sequence at either end of the unwound right-handed DNA double helix. As previously observed in the structure of triostin A-d(CGTACG) complex (A.H.-J. Wang, et. al., Science, 225, 1115-1121 (1984)), the alanine amino acid residues of the drug molecule form sequence-specific hydrogen bonds to guanines in the minor groove. The two central A.T base pairs are in Hoogsteen configuration with adenine in the syn conformation. In addition, the two terminal G.C base pairs flanking the quinoxaline rings are also held together by Hoogsteen base pairing. This is the first observation in an oligonucleotide of. Hoogsteen G.C base pairs where the cytosine is protonated. The principal functional components of a bis-intercalative compound are discussed.     

Structural studies of DNA fragments: the G.T wobble base pair in A, B and Z DNA; the G.A base pair in B-DNA

The crystal structures of five double helical DNA fragments containing non-Watson-Crick complementary base pairs are reviewed. They comprise four fragments containing G.T base pairs: two deoxyoctamers d(GGGGCTCC) and d(GGGGTCCC) which crystallise as A type helices; a deoxydodecamer d(CGCGAATTTGCG) which crystallises in the B-DNA conformation; and the deoxyhexamer d(TGCGCG), which crystallises as a Z-DNA helix. In all four duplexes the G and T bases form wobble base pairs, with bases in the major tautomer forms and hydrogen bonds linking N1 of G with O2 of T and O6 of G with N3 of T. The X-ray analyses establish that the G.T wobble base pair can be accommodated in the A, B or Z double helix with minimal distortion of the global conformation. There are, however, changes in base stacking in the neighbourhood of the mismatched bases. The fifth structure, d(CGCGAATTAGCG), contains the purine purine mismatch G.A where G is in the anti and A in the syn conformation. The results represent the first direct structure determinations of base pair mismatches in DNA fragments and are discussed in relation to the fidelity of replication and mismatch recognition.     

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.     

Interactions of Quinoxaline Antibiotic and DNA.: The Molecular Structure of a Triostin A—d(GCGTACGC) Complex

Abstract

The crystal structure of a DNA. octamer d(GCGTA.CGC) complexed to an antitumor antibiotic, triostin A, has been solved and refined to 2.2 Å resolution by x-ray diffraction analysis. The antibiotic molecule acts as a true bis intercalator surrouding the d(CpG) sequence at either end of the unwound right-handed DNA. double helix. A.s previously observed in the structure of triostin A.—d(CGTA.CG) complex (A.H.-J. Wang, et. al., Science, 225,1115–1121 (1984)), the alanine amino acid residues of the drug molecule form sequence-specific hydrogen bonds to guanines in the minor groove. The two central A · T base pairs are in Hoogsteen configuration with adenine in the syn conformation. In addition, the two terminal G · C base pairs flanking the quinoxaline rings are also held together by Hoogsteen base pairing. This is the first observation in an oligonucleotide of. Hoogsteen G · C base pairs where the cytosine is protonated. The principal functional components of a bis-intercalative compound are discussed.     

Three-dimensional structures of bulge-containing DNA fragments.

The three-dimensional structure of a DNA tridecamer d(CGCAGAATTCGCG)2 containing bulged adenine bases was determined by single crystal X-ray diffraction methods, at 120 K, to 2.6 A resolution. The structure is a B-DNA type double helix with a single duplex in the asymmetric unit. One of the bulged adenine bases loops out from the double helix, while the other stacks in to it. This is in contrast to our preliminary finding, which indicated that both adenine bases were looped out. This revised model was confirmed by the use of a covalently bound heavy-atom derivative. The conformation of the looped-out bulge hardly disrupts base stacking interactions of the bases flanking it. This is achieved by the backbone making a "loop-the-loop" curve with the extra adenine flipping over with respect to the other nucleotides in the strand. The looped-out base intercalates into the stacked-in bulge site of a symmetrically related duplex. The looped-out and stacked-in bases form an A.A reversed Hoogsteen base-pair that stacks between the surrounding base-pairs, thus stabilizing both bulges. The double helix is frayed at one end with the two "melted" bases participating in intermolecular interactions. A related structure, of the same tridecamer, after soaking the crystals with proflavin, was determined to 3.2 A resolution. The main features of this B-DNA duplex are basically similar to the native tridecamer but differ in detail especially in the conformation of the bulged-out base. Accommodation of a large perturbation such as that described here with minimal disruption of the double helix shows both the flexibility and resiliency of the DNA molecule.     

Solution structure of DAPI selectively bound in the minor groove of a DNA T.T mismatch-containing site: NMR and molecular dynamics studies.

The solution structure of the complex between 4', 6-diamidino-2-phenylindole (DAPI) and DNA oligomer [d(GCGATTCGC)]2, containing a central T.T mismatch, has been characterized by combined use of proton one- and two-dimensional NMR spectroscopy, molecular mechanics and molecular dynamics computations including relaxation matrix refinement. The results show that the DAPI molecule binds in the minor groove of the central region 5'-ATT-3' of the DNA oligomer, which predominantly adopts a duplex structure with a global right-handed B-like conformation. In the final models of the complex, the DAPI molecule is located nearly isohelical with its NH indole proton oriented towards the DNA helix axis and forming a bifurcated hydrogen bond with the carbonyl O2 groups of a mismatched T5 and the T6 residue of the opposite strand. Mismatched thymines adopt a wobble base pair conformation and are found stacked between the flanking base pairs, inducing only minor local conformational changes in global duplex structure. In addition, no other binding mechanisms were observed, showing that minor groove binding of DAPI to the mismatch-containing site is favoured in comparison with any other previously reported interaction with G.C sequences.     

Possible conformations of double-helical polynucleotides containing incorrect base pairs

Theoretical conformational analysis using classical potential functions has shown the possibility of incorporation of nucleotide mispairs with the bases in normal tautomeric forms into the DNA double helix. Incorrect purine-pyrimidine, purine-purine and pyrimidine-pyrimidine pairs can be incorporated into the double helix existing both in A- and B-conformations. The most energy favourable conformations of fragments containing a mispair have all the dihedral angles of the sugar-phosphate backbone within the limits characteristic of double helices consisting of Watson-Crick nucleotide pairs. Incorporation of mispairs is possible practically without the appearance of reduced interatomic contacts. Mutual position of bases in the incorporated mispair does not differ much from their position at the energy minimum of the corresponding isolated base pairs. Conformational parameters of irregular regions of double-stranded polynucleotides containing G:U, I:A, I:A* (syn) and U:C pairs are presented. Distortion of the sugar-phosphate backbone is the least upon incorporation of the G:U pair. Formation of mispairs in the processes of nucleic acid biosynthesis and spontaneous mutagenesis is discussed.     

Structural Studies of DNA Fragments: The G·T Wobble Base Pair in A,B and Z DNA; The G·A Base Pair in B-DNA

Abstract

The crystal structures of five double helical DNA fragments containing non-Watson-Crick complementary base pairs are reviewed. They comprise four fragments containing G·T base pairs: two deoxyoctamers d(GGGGCTCC) and d(GGGGTCCC) which crystallise as A type helices; a deoxydodecamer d(CGCGAATTTGCG) which crystallises in the B-DNA conformation; and the deoxyhexamer d(TGCGCG), which crystallises as a Z-DNA helix. In all four duplexes the G and T bases form wobble base pairs, with bases in the major tautomer forms and hydrogen bonds linking N1 of G with 02 of T and 06 of G with N3 of T. The X-ray analyses establish that the G·T wobble base pair can be accommodated in the A, B or Z double helix with minimal distortion of the global conformation. There are, however, changes in base stacking in the neighbourhood of the mismatched bases. The fifth structure, d(CGCGAATTAGCG), contains the purine purine mismatch G·A where G is in the anti and A in the syn conformation. The results represent the first direct structure determinations of base pair mismatches in DNA fragments and are discussed in relation to the fidelity of replication and mismatch recognition.     

G . T base-pairs in a DNA helix: the crystal structure of d(G-G-G-G-T-C-C-C)

The synthetic deoxyoctanucleotide d(G-G-G-G-T-C-C-C) crystallizes as an A-type DNA double helix containing two adjacent G . T base-pair mismatches. The structure has been refined to an R-factor of 14% at 2.1 A resolution with 104 solvent molecules located. The two G . T mismatches adopt the "wobble" form of base-pairing. The mismatched bases are linked by a network of water molecules interacting with the exposed functional groups in both the major and minor grooves. The presence of two mispaired bases in the octamer has surprisingly little effect on the global structure of the helix or the backbone and glycosidic torsional angles. Base stacking around the mismatch is perturbed, but the central G-T step shows particularly good base overlap, which may contribute to the relatively high stability of this oligomer.     

Refined crystal structure of an octanucleotide duplex with G . T mismatched base-pairs

Single crystal X-ray diffraction techniques have been used to determine the structure of the DNA octamer d(G-G-G-G-C-T-C-C) at a resolution of 2.25 A. The asymmetric unit consists of two strands coiled about each other to produce an A-type DNA helix. The double helix contains six G . C Watson-Crick base-pairs and two G . T mismatched base-pairs. The mismatches adopt a "wobble" type structure in which both bases retain their major tautomer forms. The double helix is able to accommodate this G . T pairing with little distortion of the overall helical conformation. Crystals of this octamer melt at a substantially lower temperature than do those of a related octamer also containing two G . T base-pairs. We attribute this destabilization to disruption of the hydration network around the mismatch site combined with changes in intermolecular packing. Full details are given of conformational parameters, base stacking, intermolecular contacts and hydration involving 52 solvent molecules.     

Refined crystal structure of an octanucleotide duplex with I.T. mismatched base pairs.

The structure of the synthetic deoxyoctamer d(GGIGCTCC) has been determined by single crystal X-ray diffraction techniques to a resolution of 1.7A. The sequence crystallises in space group P6(1), with unit cell dimensions a = b = 45.07, c = 45.49A. The refinement converged with a crystallographic residual R = 0.14 and the location of 81 solvent molecules. The octamer forms an A-DNA duplex with 6 Watson-Crick (G.C) base pairs and 2 inosine-thymine (I.T) pairs. Refinement of the structure shows it to be essentially isomorphous with that reported for d(GGGGCTCC) with the mispairs adopting a "wobble" conformation. Conformational parameters and base stacking interactions are compared to those for the native duplex d(GGGGCCCC) and other similar sequences. A rationale for the apparent increased crystal packing efficiency and lattice stability of the I.T octamer is given.     

Thermodynamics of DNA duplexes with adjacent G.A mismatches.

The sequence 5'-d(ATGAGCGAAT) forms a very stable self-complementary duplex with four G.A mismatch base pairs (underlined) out of ten total base pairs [Li et al. (1991) Proc. Natl. Acad. Sci. U.S.A. 88, 26-30]. The conformation is in the general B-family and is stabilized by base-pair hydrogen bonding of an unusual type, by favorable base dipole orientations, and by extensive purine-purine stacking at the mismatched sites. We have synthesized 13 decamers with systematic variations in the sequence above to determine how the flanking sequences, the number of G.A mismatches, and the mismatch sequence order (5'-GA-3' or 5'-AG-3') affect the duplex stability. Changing A.T to G.C base pairs in sequences flanking the mismatches stabilizes the duplexes, but only to the extent observed with B-form DNA. The sequence 5'-pyrimidine-GA-purine-3', however, is considerably more stable than 5'-purine-GA-pyrimidine-3'. The most stable sequences with two pairs of adjacent G.A mismatches have thermodynamic parameters for duplex formation that are comparable to those for fully Watson-Crick base-paired duplexes. Similar sequences with single G.A pairs are much less stable than sequences with adjacent G.A mismatches. Reversing the mismatch order from 5'-GA-3' to 5'-AG-3' results in an oligomer that does not form a duplex. These results agree with predictions from the model derived from NMR and molecular mechanics and indicate that the sequence 5'-pyrimidine-GA-purine-3' forms a stable conformational unit that fits quite well into a B-form double helix.(ABSTRACT TRUNCATED AT 250 WORDS)     

An approach to the structure determination of nucleic acid analogues hybridized to RNA. NMR studies of a duplex between 2'-OMe RNA and an oligonucleotide containing a single amide backbone modification.

The backbone modification amide-3, in which -CH2-NH-CO-CH2- replaces -C5'H2-O5'-PO2-O3'-, is studied in the duplex d(G1-C2-G3-T4.T5-G6-C7-G8)*mr(C9-G10-C11-A12-A13-C14-G15+ ++-C16) where . indicates the backbone modification and mr indicates the 2'-OMe RNA strand. The majority of the exchangeable and non-exchangeable resonances have been assigned. The assignment procedure differs from standard methods. The methyl substituent of the 2'-OMe position of the RNA strand can be used as a tool in the interpretation. The duplex structure is a right-handed double helix. The sugar conformations of the 2'-OMe RNA strand are predominantly N-type and the 2'-OMe is positioned at the surface of the minor groove. In the complementary strand, only the sugar of residue T4 is found exclusively in N-type conformation. The incorporation of the amide modification does not effect very strongly the duplex structure. All bases are involved in Watson-Crick base pairs.     

Crystal structures of A-DNA duplexes

All crystal structures of A-DNA duplexes exhibit a typical crystal packing, with the termini of one molecule abutting the shallow grooves of symmetry related neighbors, while all other forms (B, Z, and RNA) tend to form infinitely stacked helices. The A-DNA arrangement leads to the formation of shallow groove base multiples that have implications for the structure of DNA in compacted states. The characteristic packing leaves big solvent channels, which can be sometimes occupied by B-DNA duplexes. Comparisons of the structures of the same oligomer crystallizing in two different space groups and of different sequences crystallizing in the same space group show that the lattice forces dominate the A-DNA conformation in the crystals, complicating the effort to elucidate the influence of the base sequence on the structures. Nevertheless, in both alternating and nonalternating fragments some sequence effects can still be uncovered. Furthermore, several studies have started to define the minimal sequence changes or chemical modifications that can interconvert the oligomers between different double-helical conformers (A-, B-, and Z-form). Overall, it is seen that the rigid nucleotide principle applies to the oligomeric fragments. Besides the structures of the naked DNAs, their interactions with water, polyamines, and metal ions have attracted considerable attention. There are conserved patterns in the hydration, involving both the grooves and the backbone, which are different from those of B-DNA or Z-DNA. Overall, A-DNA seems to be more economically hydrated than B-DNA, particularly around the sugar-phosphate backbone. Spermine was found to be able to bind exclusively to either of the grooves or to the phosphate groups of the backbone, or exhibit a mixed binding mode. The located metal cations prefer binding to guanine bases and phosphate groups. The only mispairs investigated in A-DNA are the wobble pairs, yielding structural insight into their effects on helix stabilities and hydration. G · T wobble pairs have been determined in various sequence contexts, where they differentially affect the conformations and stableness of the duplexes. The structure of a G · ^m5C base pair, which surprisingly also adopted the wobble conformation, suggests that a similar geometry may transiently exist for G · C pairs. These results from the crystalline state will be compared to the solution state and discussed in relation to their relevance in biology. © 1997 John Wiley & Sons, Inc. Biopoly 44: 45–63, 1997     

Structural features and hydration of d(C-G-C-G-A-A-T-T-A-G-C-G); a double helix containing two G.A mispairs

Single crystal X-ray diffraction techniques have been used to characterise the molecular structure of the title compound to 2.5A resolution. The structure consists of ten standard Watson-Crick base pairs and two G.A mismatched base pairs. The purine-purine mismatches have guanine in the usual anti orientation with respect to the sugar and adenine in syn orientation. There are two hydrogen bonds formed between the mismatch bases, N-1 and O-6 of guanine with N-7 and N-6 of adenine respectively. The bulky purine-purine mismatches are accommodated with minor perturbation of the sugar-phosphate backbone. There is a slight improvement in base pair overlap at the mismatch sites. Details of the backbone conformation, base stacking interactions and hydration are presented and compared with those of the parent compound d(C-G-C-G-A-A-T-T-C-G-C-G).     

Inosine.adenine base pairs in a B-DNA duplex.

The structure of the synthetic deoxydodecamer d(C-G-C-I-A-A-T-T-A-G-C-G) has been determined by single crystal X-ray diffraction techniques at 2.5A resolution. The refinement converged with a crystallographic residual, R = 0.19 and the location of 64 solvent molecules. The sequence crystallises as a B-DNA helix with 10 Watson-Crick base-pairs (4 A.T. and 6 G.C) and 2 inosine.adenine (I.A) pairs. The present work shows that in the purine.purine base-pairs the adenine adopts syn orientation with respect to the furanose moiety while the inosine is in the trans (anti) orientation. Two hydrogen bonds link the I.A. base-pair, one between N-1(I) and N-7(A), the other between O-6(I) and N-6(A). This bulky purine.purine base-pair is incorporated in the double helix at two positions with little distortion of either local or global conformation. The pairing observed in this study is presented as a model for I.A base-pairs in RNA codon-anticodon interactions and may help explain the thermodynamic stability of inosine containing base-pairs. Conformational parameters and base stacking interactions are presented and where appropriate compared with those of the native compound, d(C-G-C-G-A-A-T-T-C-G-C-G) and with other studies of oligonucleotides containing purine.purine base-pairs.     

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.     

Three-dimensional structure of d(GGGATCCC) in the crystalline state.

The structure of the self-complementary octamer d(GGGATCCC) has been analysed by single crystal X-ray diffraction methods at a nominal resolution of 2.5 A. With acceptable stereochemistry of the model the crystallographic R factor was 16.6% after restrained least-squares refinement. In the crystal, d(GGGATCCC) forms an A-DNA double helix with slightly varying conformation of the two strands. The average displacement of the base pairs from the helix axis is unusually large and is accompanied by pronounced sliding of the base pairs along their long axes at all dinucleotide steps except for the central AT. With 12 base pairs per complete turn the helix is considerably underwound. As observed with most oligodeoxyribonucleotides analysed by X-ray crystallography so far, the octamer displays reduced base pair tilt, increased rise per base pair and a more open major groove compared with canonical A-DNA. We propose that, based on these parameters, three A-helical sub-families may be defined; d(GGGATCCC) then is a representative of the class with intermediate tilt, rise, and major groove width.