Fibre-type X-ray diffraction patterns from single crystals of triple helical DNA

Enhanced stabilization of the triplexes d(C(+)-T)(6):d(A-G)(6);d(C-T)(6), d(T)(21):d(A)(21);d(T)(21) and poly r(U:AU) by water structure-making solutes

A variety of organic cations, cationic lipids, low molecular weight alcohols, sodium dodecylsulfate, trehalose, glycerol, low molecular weight polyethylene glycols, and DMSO were tested for their ability to modulate the stability of the triplexes d(C(+)-T)(6):d(A-G)(6);d(C-T)(6), d(T)(21):d(A)(21);d(T)(21), poly r(U:A U) and their respective core duplexes, d(A-G)(6);d(C-T)(6), d(A)(21);d(T)(21), poly r(A-U). Very substantial enhancement of triplex stability over that in a physiological salt buffer at pH 7 is obtained with different combinations of triplex and high concentrations of these additives, e.g. trimethylammonium chloride and d(C(+)-T)(6):d(A-G)(6);d(C-T)(6); 2-propanol and d(T)(21):d(A)(21);d(T)(21); ethanol and poly r(U:A;U). Triplex formation is even observed with a 1:1 strand mixture of d(A-G)(6) and d(C-T)(6) in the presence of dimethylammonium, tetramethylammonium, and tetraethylammonium-chloride, as well as methanol, ethanol, and 2-propanol. Triplex stability follows the water structure-making ability (and in some cases the duplex unwinding ability) of the organic cations, the low molecular weight alcohols and other neutral organic compounds, whereas water structure-breaking additives decrease triplex stability. These findings are consistent with those reported in the accompanying paper that triplex formation occurs with a net uptake of water. Since the findings suggest that third strand-binding is facilitated by unwinding of the target duplex, it is inferred that triplex formation may be enhanced by nucleic acid binding proteins operating similarly.

Structure-function relationship of three triple-helical nucleic acids

The nucleic acid triplexes poly d(T) x poly d(A) x poly d(T), poly (U) x poly (A) x poly (U), and poly (I) x poly (A) x poly (I) display a sort of continuity between each other. However, their morphologies present their own individuality which, considering those of their parent duplexes, are quite unexpected. This comparison helps to understand triplex structure-function relationship. While helical parameters are functions of the sugar pucker, low values of WC and Hoogsteen base-pair propellers is commonplace for triplexes and the Hoogsteen base-pair geometry monitors the effects of the interstrand phosphates charge-charge repulsion.

Structure of poly (dT).poly (dA).poly (dT)

The molecular structure of poly (dT).poly (dA).poly (dT) has been determined and refined using the continuous x-ray intensity data on layer lines in the diffraction pattern obtained from an oriented fiber of the DNA. The final R-value for the preferred structure is 0.29 significantly lower than that for plausible alternatives. The molecule forms a 12-fold right-handed triple-helix of pitch 38.4 A and each base triplet is stabilized by a set of four Crick-Watson-Hoogsteen hydrogen bonds. The deoxyribose rings in all the three strands have C2'-endo conformations. The grooveless cylindrical shape of the triple-helix is consistent with the lack of lateral organization in the fiber.

Free energy of the binding of uridylic acid oligomers with double stranded poly(A) · poly(U)

The binding parameters (K, omega) and the free energy (DeltaG(0)) of triple helix formation have been estimated for complexes of oligo(U)(n) (n = 5, 7-10) with poly(A) . poly(U) on the basis of hypochromicity measurements. The data were treated according to the formula of McGhee and von Hippel [J. Mol. Biol. 86 (1974) 469] by a computer program ALAU [H. Schütz et al., Stud. Biophys. 104 (1984) 23] which takes absorbancies and total concentrations as input. In 1 mM cacodylate buffer pH 7.0 with 10 mM NaCl and 10 mM MgCl(2) at 5 degrees C the free energy of contiguous binding was found to be a linear function of the oligomer length with a slope of DeltaG(c,U)(0) = -0.72 (+/-0.03) kcal x mol(-1) per nucleotide. The mean cooperativity coefficient (omega) was 24.5 (+/- 5.6), and the corresponding free energy of interaction between the neighbouring oligonucleotides in the third strand was DeltaG(0(omega)) = -1.74 (+/-0.13) kcal x mol(-1).

Homopurine and homopyrimidine strands complementary in parallel orientation form an antiparallel duplex at neutral pH with A-C, G-T, and T-C mismatched base pairs

DNA sequences d-TGAGGAAAGAAGGT (a 14-mer) and d-CTCCTTTCTTCC (a 12-mer) are complementary in parallel orientation forming either Donohue (reverse Watson-Crick) base pairing at neutral pH or Hoogsteen base pairing at slightly acidic pH. The structure of the complex formed by dissolving the two strands in equimolar ratio in water has been investigated by nmr. At neutral pH, the system forms an ordered antiparallel duplex with five A : T and four G : C Watson-Crick base pairs and three mismatches, namely G-T, A-C, and T-C. The nuclear Overhauser effect cross-peak pattern suggests an overall B-DNA conformation with major structural perturbations near the mismatches. The duplex has a low melting point and dissociates directly into single strands with a broad melting profile. The hydrogen-bonding schemes in the mismatched base pairs have been investigated. It has been shown earlier that in acidic pH, the system prefers a triple-stranded structure with two pyrimidine strands and one purine strand. One of the pyrimidine strands has protonated cytosines, forms Hoogsteen base pairing, and is aligned parallel to the purine strand; the other has nonprotonated cytosines and has base-pairing scheme similar to the one discussed in this paper. The parallel duplex is therefore less stable than either the antiparallel duplex or the triplex, in spite of its perfect complementarity.

Novel Hoogsteen-like bases for configurational recognition of the T-A base pair by DNA triplex formation

Effective sequence-specific recognition of duplex DNA is possible by triplex formation with natural oligonucleotides via Hoogsteen H-bonding. However, triplex formation is in practice limited to pyrimidine oligonucleotides binding duplex A-T or G-C base-pair DNA sequences specifically at homopurine sites in the major groove as T-A-T and C+.G-C triplets. Here we report the successful modeling of novel unnatural nucleosides that recognize the T-A DNA base pair by Hoogsteen interaction. Since the DNA triplex can be considered to assume an A-type or B-type conformation, these novel Hoogsteen nucleotides are tested within model A-type and B-type conformation triplex structures. A triplet consisting of the T-A base pair and one of the novel Hoogsteen nucleotides replaces the central T.A-T triplet in the triplex using the same deoxyribose-phosphodiester and base-deoxyribose dihedral angle configuration. The entire triplex is energy minimized and the presence of any structural or energetic perturbations due to the central triplet is assessed with respect to the unmodified energy-minimized (T.A-T)11 proposed starting structures. Incorporation of these novel triplets into both A-type and B-type natural tiplex structures provokes minimal change in the configuration of the central and adjacent triplets. The plan is to produce a series of Hoogsteen-like bases that preferentially bind the T-A major groove in either an A-type or B-type conformation. Selective recognition of the T-A major groove with respect to the G-C major groove, which presents similar keto and amine placement, is also assessed with configurational preference. Evaluation of the triplex solution structure by using these unnatural bases as binding conformational probes is a prerequisite to the further design of triplet forming bases.

Structure of Py.Pu.Py DNA triple helices. Fourier transforms of fiber-type x-ray diffraction of single crystals

Well-formed hexagonal crystals of oligomeric DNA triple helices exhibit fiber-type x-ray diffraction patterns [cf., Liu et al. (1994) Nature Struct. Biol. 1, 11], which can be interpreted in terms of Fourier transforms of these helices. Precession photographs of a triplex formed of dA and dT chains show that it has 13 residues per turn. In contrast, a sequence containing the four natural bases A, G, C, and T has 12 residues per turn. In this sense the triple helices exhibit a sequence-dependent polymorphism, though both have C2'-endo sugar pucker and B rather than A conformation. New models are constructed, using constraints from x-ray diffraction, and Fourier transforms of the models are calculated. Good agreement in the amplitudes and positions of the calculated and observed diffraction intensities confirms the structures for both triple helices. These are the first stereochemically satisfactory DNA triple helices for which coordinates based on adequate experimental data were provided. Sequences for crystallization are designed to achieve unique base alignments and are screened for the presence of sharp bands on gel electrophoresis to assure the absence of multiple species caused by strand slippage. Despite intensive efforts to observe normal crystal diffraction by varying sequences and conditions, all crystals exhibited only fiber-type diffraction. We suggest that this behavior may be an intrinsic property of triple helices and discuss possible reasons for the results. Spectroscopic and chemical experiments establish that the oligonucleotides exist in solution as triple helices under the conditions of crystallization.

Parallel and antiparallel (G.GC)2 triple helix fragments in a crystal structure

Nucleic acid triplexes are formed by sequence-specific interactions between single-stranded polynucleotides and the double helix. These triplexes are implicated in genetic recombination in vivo and have application to areas that include genome analysis and antigene therapy. Despite the importance of the triple helix, only limited high-resolution structural information is available. The x-ray crystal structure of the oligonucleotide d(GGCCAATTGG) is described; it was designed to contain the d(G middle dotGC)2 fragment and thus provide the basic repeat unit of a DNA triple helix. Parameters derived from this crystal structure have made it possible to construct models of both parallel and antiparallel triple helices.

Simultaneous binding of a polyamide dimer and an oligonucleotide in the minor and major grooves of DNA

The effect of the polyamide ImPyPy-Dp (Im = N-methylimidazole-2-carboxamide, Py = N-methylpyrrole-2-carboxamide, and Dp = dimethylaminopropylamide), which binds as an antiparallel dimer in the Watson-Crick minor groove, on pyrimidine. purine.pyrimidine triple helix stability was investigated. A DNA restriction fragment was designed which contained two triple helix sites, one which overlapped a minor groove ligand site (proximal), and a control site 13 base pairs away (distal). Using quantitative DNase I footprint titration experiments the equilibrium association constant of oligonucleotide 5'-TTTTTm5CTTTm5CTTTm5CT-3' (1) to each site was measured in the absence and presence of the polyamide dimer. Our data indicate that triple helix formation is compatible with a polyamide dimer binding in the minor groove of DNA at an overlapping site. No cooperative effect of the polyamide dimer on the equilibrium association constant of oligonucleotide 1 was observed.

Symmetry and structure of RNA and DNA triple helices

Despite wide interest in nucleic acid triple helices, there has been no stereochemically satisfactory structure of an RNA triple helix in atomic detail. AN RNA triplex structure has previously been proposed based on fiber diffraction and molecular modeling [S. Arnott and P. J. Bond (1973) Nature New Biology, Vol. 244, pp. 99-101; S. Arnott, P. J. Bond, E. Selsing, and P. J. C. Smith (1976) Nucleic Acids Research, Vol. 3, pp. 2459-2470], but it has nonallowed close contacts at every triplet and is therefore not stereochemically acceptable. We propose here a new model for an RNA triple helix in which the three chains have identical backbone conformations and are symmetry related. There are no short contacts. The modeling employs a novel geometrical approach using the linked atom least squares [P. J. C. Smith and S. Arnott (1978) Acta Crystallographica, Vol. A34, pp. 3-11] program and is not based on energy minimization. In general, the method leads to a range of possible structures rather than a unique structure. In the present case, however, the constraints resulting from the introduction of a third strand limit the possible structures to a very small range of conformation space. This method was used previously to obtain a model for DNA triple helices [G. Raghunathan, H. T. Miles, and V. Sasisekharan (1993) Biochemistry, Vol. 32, pp. 455-462], subsequently confirmed by fiber-type x-ray diffraction of oligomeric crystals [K. Liu, H. T. Miles, K. D. Parris, and V. Sasisekharan (1994) Nature Structural Biology, Vol. 1, pp. 11-12]. The above triple helices have Watson-Crick-Hoogsteen [K. Hoogsteen (1963) Acta Crystallographica, Vol. 16, pp. 907-916] pairing of the three bases. The same modeling method was used to investigate the feasibility of three-dimensional structures based on the three possible alternative hydrogen-bonding schemes: Watson-Crick-reverse Hoogsteen, Donohue [J. Donohue (1953) Proceedings of the National Academy of Science USA, Vol. 39, pp. 470-475] (reverse Watson-Crick)-Hoogsteen, and Donohue-reverse Hoogsteen. We found that none of these can occur in either RNA or DNA helices because they give rise only to structures with prohibitively short contacts between backbone and base atoms in the same chain.

New crystal structures of nucleic acids and their complexes

In the past year, X-ray crystallographic studies of representatives of all nucleic acid structural types have been reported. Among the most interesting structures are the parallel DNA tetraplex formed by d(TGGGGT), the four-stranded structure formed by d(CCCT) and a double drug bound side by side in an antiparallel orientation to the minor groove of a B-DNA. Certainly, the structure that has received most attention is that of the first complex of a ribozyme with an inhibitor DNA.

Solvent effects on model d(CG.G)7 and d(TA.T)7 DNA triple helices

Using free energy molecular mechanics, we find that the molecular effects of solvent are critical in determining relative stabilities in DNA triple helices or triplexes. The continuum solvent model is unable to differentiate the thermodynamics reflecting the basic solvation differences around the occupied major groove in triplexes. In order to avoid the local minimum problem, which is a major limitation of any modeling study, we started our computations with multiple structures rather than relying on the optimization of a single reference structure. By constructing triplex models with different initial helical twists, helical rises, and sugar-pucker permutations, we explore the potential surface and the structural preference with respect to these variations. We find that in order to accommodate a third strand in triplex formation, the backbone geometry of the B-DNA duplex target has to be adjusted into A-DNA-like form with a deep major groove. This is achieved by concerted adjustment in torsions beta, epsilon, and zeta around the phosphate groups. However, the sugar pucker displays a more rich variation, resulting in conformations not usually associated with the canonical duplex structures.