Spectroscopic studies on ethidium bromide binding to intramolecular parallel and antiparallel triple helices containing T*A:T and G*G:C triplets

The interaction of ethidium bromide (EB), a DNA intercalator, with two intramolecular triplexes 5'd(G4A4G4-[T4]-C4T4C4-[T4]-G4T4G4), 5'd(G4T4G4-[T4]-G4A4G4-[T4]-C4T4C4) ([T4] represents a stretch of 4 thymine residues) and their precursor duplexes has been investigated by circular dichroism, fluorescence and UV absorption spectroscopy. Binding of EB induces a circular dichroism band in the region around 310 nm which is positive for the duplex forms but negative for the triplex forms. We observed that the binding of EB to the duplex form does not induce the formation of the triplex structures. Thermal denaturation experiments demonstrate that EB stabilizes more the parallel triple helix than the antiparallel one. Analysis of the binding process from fluorescence measurements shows that binding constants to the triple helical forms and to the hairpin reference duplex [T4]-G4A4G4-[T4]-C4T4C4) are close. However the binding site size is larger for the triplexes (4-6 base triplets) than for the duplex (2 base pairs).     

Molecular dynamics simulations on parallel and antiparallel C.G*G triplexes

Molecular dynamics (MD) studies have been carried out on the Hoogsteen hydrogen bonded parallel and the reverse Hoogsteen hydrogen bonded antiparallel C.G*G triplexes. Earlier, the molecular mechanics studies had shown that the parallel structure was energetically more favourable than the antiparallel structure. To characterize the structural stability of the two triplexes and to investigate whether the antiparallel structure can transit to an energetically more favourable structure, due to the local fluctuations in the structure during the MD simulation, the two structures were subjected to 200ps of constant temperature vacuum MD simulations at 300K. Initially no constraints were applied to the structures and it was observed that for the antiparallel triplex, the structure showed a large root mean square deviation from the starting structure within the first 12ps and the N4-H41--O6 hydrogen bond in the WC duplex got distorted due to a high propeller twist and a moderate increase in the opening angle in the basepairs. Starting from an initial value of 30 degrees , helical twist of the average structure from this simulation had a value of 36 degrees , while the parallel structure stabilized at a twist of 33 degrees. In spite of the hydrogen bond distortions in the antiparallel triplex, it was energetically comparable to the parallel triplex. To examine the structural characteristics of an undistorted structure, another MD simulation was performed on the antiparallel triplex by constraining all the hydrogen bonds. This structure stabilized at an average twist of 33 degrees. In the course of the dynamics though the energy of the molecule - compared to the initial structure - improved, it did not become comparable to the parallel structure. Energy minimization studies performed in the presence of explicit water and counterions also showed the two structures to be equally favourable energetically. Together these results indicate that the parallel C.G*G triplex with Hoogsteen hydrogen bonds also represents a stereochemically and energetically favourable structure for this class of triplexes.     

Thermodynamic and kinetic stability of intermolecular triple helices containing different proportions of C+*GC and T*AT triplets

We have used oligonucleotides containing appropriately placed fluorophores and quenchers to measure the stability of 15mer intermolecular triplexes with third strands consisting of repeats of TTT, TTC, TCC and TCTC. In the presence of 200 mM sodium (pH 5.0) triplexes that contain only T·AT triplets are unstable and melt below 30°C. In contrast, triplets with repeats of TTC, TCC and CTCT melt at 67, 72 and 76°C, respectively. The most stable complex is generated by the sequence containing alternating C⁺·GC and T·AT triplets. All four triplexes are stabilised by increasing the ionic strength or by the addition of magnesium, although triplexes with a higher proportion of C⁺·GC triplets are much less sensitive to changes in the ionic conditions. The enthalpies of formation of these triplexes were estimated by examining the concentration dependence of the melting profiles and show that, in the presence of 200 mM sodium at pH 5.0, each C⁺·GC triplet contributes about 30 kJ mol^–1, while each T·AT contributes only 11 kJ mol^–1. Kinetic experiments with these oligonucleotides show that in 200 mM sodium (pH 5.0) repeats of TCC and TTC have half-lives of ~20 min, while the triplex with alternating C⁺·GC and T·AT triplets has a half-life of ~3 days. In contrast, the dissociation kinetics of the triplex containing only T·AT are too fast to measure.     

Site-resolved energetics in DNA triple helices containing G*TA and T*CG triads

Recognition of specific sites in double-helical DNA by triplex-forming oligonucleotides has been limited until recently to sites containing homopurine-homopyrimidine sequences. G*TA and T*CG triads, in which TA and CG base pairs are specifically recognized by guanine or by thymine, have now extended this recognition code to DNA target sites of mixed base sequences. In the present work, we have obtained a characterization of the stabilities of G*TA and T*CG triads, and of the effects of these triads upon canonical triads, in triple-helical DNA. The three DNA triplexes investigated are formed by the folding of the 31-mers d(GAAXAGGT(5)CCTYTTCT(5)CTTZTCC) with X = G, T, or C, Y = C, A, or G, and Z = C, G, or T. We have measured the exchange rates of imino protons in each triad of the three triplexes using nuclear magnetic resonance spectroscopy. The exchange rates are used to map the local free energy of structural stabilization in each triplex. The results indicate that the stability of Watson-Crick base pairs in the G*TA and T*CG triads is comparable to that of Watson-Crick base pairs in canonical triads. The presence of G*TA and T*CG triads, however, destabilizes neighboring canonical triads, two or three positions removed from the G*TA/T*CG site. Moreover, the long-range destabilizing effects induced by the T*CG triad are larger than those induced by the G*TA triad. These findings reveal the molecular basis for the lower overall stability of G*TA- and T*CG-containing triplexes.     

Alternating d(GA)n DNA sequences form antiparallel stranded homoduplexes stabilized by the formation of G.A base pairs.

Alternating d(GA)n DNA sequences form antiparallel stranded homoduplexes which are stabilized by the formation of G.A pairs. Three base pairings are known to occur between adenine and guanine: AH+ (anti).G(syn), A(anti).G(anti) and A(syn).G(anti). Protonation of the adenine residues is not involved in the stabilization of this structure, since it is observed at any pH value from 8.3 to 4.5; at pH < or = 4.0 antiparallel stranded d(GA.GA) DNA is destabilized. The results reported in this paper strongly suggest that antiparallel stranded d(GA.GA) homoduplexes are stabilized by the formation of alternating A(anti).G(anti) and G(anti).A(syn) pairs. In this structure, all guanine residues are in the anti conformation with their N7 position freely accessible to DMS methylation. On the other hand, adenines in one strand adopt the anti conformation, with their N7 position also free for reaction, while those of the opposite strand are in the syn conformation, with their N7 position hydrogen bonded to the guanine N1 group of the opposite strand. A regular right-handed helix can be generated using alternating G(anti).A(syn) and A(anti).G(anti) pairs.     

Formation of DNA triple helices incorporating blocks of G.GC and T.AT triplets using short acridine-linked oligonucleotides.

We have used DNase I footprinting to assess triple helix formation at target sites containing the sequences A6G6.C6T6 and G6A6.T6C6. These sequences can be recognized by the acridine-linked oligopyrimidines Acr-T5C5 and Acr-C5T5 respectively at low pH, using well-characterised T.AT and C+.GC triplets. At pH 7.5 A6G6.C6T6 is specifically bound by Acr-G5T5, utilising G.GC and T.AT triplets in which the third strand runs antiparallel to the purine strand of the duplex. This interaction requires the presence of magnesium ions. No interaction was detected with Acr-T5G5, an oligonucleotide designed to form parallel G.GC and T.AT triplets. In contrast neither Acr-T5G5 nor Acr-G5T5 produced DNase I footprints with the target sequence G6A6.T6C6. These results suggest that, in an antiparallel R.RY triple helix, the T.AT triplet is weaker than the G.GC triplet. We find no evidence for the formation of structures containing parallel G.GC triplets.     

Circular dichroism measurements show that C.C+ base pairs can coexist with A.T base pairs between antiparallel strands of an oligodeoxynucleotide double-helix.

We have studied the coil-to-helix transition of the DNA oligomer d(C4A4T4C4), using circular dichroism measurements to monitor the formation of A.T base pairs within the central self-complementary A4T4 region and the formation of protonated C.C+ base pairs at the ends of the oligomer. We found that both A.T and C.C+ base pairs formed in a coordinated fashion as the temperature and pH were lowered. The CD data of the helix form of the oligomer were consistent with the presence of paired oligomers, but not with hairpin loops. The pKa for formation of C.C+ base pairs between the C4 ends of the oligomer was higher than the pKa for formation of C.C+ base pairs in d(C8), indicating that the formation of C.C+ base pairs in the oligomer was influenced by the presence of a paired A4T4 region. We conclude that A.T and C.C+ base pairs coexist in the self-complex of the oligomer and, therefore, that C.C+ base pairs can form between antiparallel DNA strands.     

Comparison of the solution structures of intramolecular DNA triple helices containing adjacent and non-adjacent CG.C+ triplets.

The solution conformations of the intramolecular triple helices d(AGAAGA-X-TCTTCT-X-TC+TTC+T) and d(AAGGAA-X-TTCCTT-X-TTC+C+TT) (X = non-nucleotide linker) have been determined by NMR.1H NMR spectra in H2O showed that the third strand cytosine residues are fully paired with the guanine residues, each using two Hoogsteen hydrogen bonds. Determination of the13C chemical shifts of the cytosine C6 and C5 and their one-bond coupling constants (1 J CH) conclusively showed that the Hoogsteen cytosine residues are protonated at N3. The global conformations of the two molecules determined with >19 restraints per residue are very similar (RMSD = 0.96 A). However, some differences in local conformation and dynamics were observed for the central two base triplets of the two molecules. The C N3H were less labile in adjacent CG.C+triplets than in non-adjacent ones, indicating that the adjacent charge does not kinetically destabilize these triplets. The sugar conformations of the two adjacent cytosine residues were different and the 5'-residue was atypical of protonated cytosine. Hence, there are subtle effects of the interaction between two adjacent cytosine residues. The central two purines in each sequence showed non-standard backbone conformations, averaging between gamma approximately 60 degrees and gamma approximately 180 degrees. This may be related to the difference in the dependence of the thermodynamic stability on pH observed for these two sequences.     

Parallel DNA helices. Conformational analysis of regular poly(dG).poly(dC) helices with different variants of base binding]

We have performed a conformational analysis of DNA double helices with parallel directed backbone strands. The calculations were made for homopolymers poly(dG).poly(dC). All possible models of base binding were checked. By the potential energy optimization the dihedral angles and helices parameters of stable conformations of parallel double polynucleotides were calculated. The dependences of conformational energy on the base pair structure were studied. Possible structure of parallel helices with various nucleotide composition are discussed.     

Parallel intramolecular DNA triple helix with G and T bases in the third strand stabilized by Zn(2+) ions

We present evidence of formation of an intramolecular parallel triple helix with T•A.T and G•G.C base triplets (where • represents the hydrogen bonding interaction between the third strand and the duplex while . represents the Watson–Crick interactions which stabilize the duplex). The third GT strand, containing seven GpT/TpG steps, targets the polypurine sequence 5′-AGG-AGG-GAG-GAG-3′. The triple helix is obtained by the folding back twice of a 36mer, formed by three dodecamers tethered by hydroxyalkyl linkers (-L-). Due to the design of the oligonucleotide, the third strand orientation is parallel with respect to the polypurine strand. Triple helical formation has been studied in concentration conditions in which native gel electrophoresis experiments showed the absence of intermolecular structures. Circular dichroism (CD) and UV spectroscopy have been used to evidence the triplex structure. A CD spectrum characteristic of triple helical formation as well as biphasic UV and CD melting curves have been obtained in high ionic strength NaCl solutions in the presence of Zn²⁺ ions. Specific interactions with Zn²⁺ ions in low water activity conditions are necessary to stabilize the parallel triplex.     

Thermodynamics of triple helix formation: spectrophotometric studies on the d(A)10.2d(T)10 and d(C+3T4C+3).d(G3A4G3).d(C3T4C3) triple helices.

We have stabilized the d(A)10.2d(T)10 and d(C+LT4C+3).d(G3A4G3).d(C3T4C3) triple helices with either NaCl or MgCl2 at pH 5.5. UV mixing curves demonstrate a 1:2 stoichiometry of purine to pyrimidine strands under the appropriate conditions of pH and ionic strength. Circular dichroic titrations suggest a possible sequence-independent spectral signature for triplex formation. Thermal denaturation profiles indicate the initial loss of the third strand followed by dissociation of the underlying duplex with increasing temperature. Depending on the base sequence and ionic conditions, the binding affinity of the third strand for the duplex at 25 degrees C is two to five orders of magnitude lower than that of the two strands forming the duplex. Thermodynamic parameters for triplex formation were determined for both sequences in the presence of 50 mM MgCl2 and/or 2.0 M NaCl. Hoogsteen base pairs are 0.22-0.64 kcal/mole less stable than Watson-Crick base pairs, depending on ionic conditions and base composition. C+.G and T.A Hoogsteen base pairs appear to have similar stability in the presence of Mg2+ ions at low pH.     

Intramolecular triple-helix formation at (PunPyn).(PunPyn) tracts: recognition of alternate strands via Pu.PuPy and Py.PuPy base triplets.

Triple-helical DNA shows increasing potential for applications in the control of gene expression (including therapeutics) and the development of sequence-specific DNA-cleaving agents. The major limitation in this technology has been the requirement of homopurine sequences for triplex formation. We describe a simple approach that relaxes this requirement, by utilizing both Pu.PuPy and Py.PuPy base triplets to form a continuous DNA triple helix at tandem oligopurine and oligopyrimidine tracts. [Triplex formation at such a sequence has been previously demonstrated only with the use of a special 3'-3' linkage in the third strand [Horne, D. A., & Dervan, P. B. (1990) J. Am. Chem. Soc. 112, 2435-2437].] Supporting evidence is from chemical probing experiments performed on several oligonucleotides designed to form 3-stranded fold-back structures. The third strand, consisting of both purine and pyrimidine blocks, pairs with purines in the Watson-Crick duplex, switching strands at the junction between the oligopurine and oligopyrimidine blocks but maintaining the required strand polarity without any special linkage. Although Mg2+ ions are not required for the formation of Pu.PuPy base triplets, they show enhanced stability in the presence of Mg2+. In the sequences observed. A.AT triplets appear to be more stable than G.GC triplets. As expected, triplex formation is largely independent of pH unless C+.GC base triplets are required.     

Triple helices formed at oligopyrimidine*oligopurine sequences with base pair inversions: effect of a triplex-specific ligand on stability and selectivity.

Oligonucleotide-directed triple helix formation is mostly restricted to oligopyrimidine*oligopurine sequences of double helical DNA. An interruption of one or two pyrimidines in the oligopurine target strand leads to a strong triplex destabilisation. We have investigated the effect of nucleotide analogues introduced in the third strand at the site opposite the base pair inversion(s). We show that a 3-nitropyrrole derivative (M) discriminates G*C from C*G, A*T and T*A in the presence of a triplex-specific ligand (a benzo[e]pyridoindole derivative, BePI). N6-methoxy-2,6-diaminopurine (K) binds to an A*T base pair better than a T*A, G*C or C*G base pair. Some discrimination is still observed in the presence of BePI and triplex stability is markedly increased. These findings should help in designing BePI-oligonucleotide conjugates to extend the range of DNA sequences available for triplex formation.     

Circular dichroism and UV melting studies on formation of an intramolecular triplex containing parallel T*A:T and G*G:C triplets: netropsin complexation with the triplex.

We have used circular dichroism and UV absorption spectroscopy to characterize the formation and melting behaviour of an intramolecular DNA triple helix containing parallel T*A:T and G*G:C triplets. Our approach to induce and to stabilize a parallel triplex involves the oligonucleotide 5'-d(G4A4G4[T4]C4T4C4-[T4]G4T4G4) ([T4] represents a stretch of four thymine residues). In a 10 mM sodium cacodylate, 0.2 mM disodium EDTA (pH 7) buffer, we have shown the following significant results. (i) While in the absence of MgCl2 this oligonucleotide adopts an intramolecular hairpin duplex structure prolonged by the single strand extremity 5'-d([T4]G4T4G4), the presence of millimolar concentrations of MgCl2generates an intramolecular triplex (via double hairpin formation). (ii) In contrast to the antiparallel triplex formed by the oligonucleotide 5'-d(G4T4G4[T4]G4A4G4[T4]C4T4C4), the parallel triplex melts in a biphasic manner (a triplex to duplex transition followed by a duplex to coil transition) and is less stable than the antiparallel one. The enthalpy change associated with triplex formation (-37 kcal/mol) is approximately half that of duplex formation (-81 kcal/mol). (iii) The parallel triple helix is disrupted by increasing the concentration of KCl(>10 mM), whereas, under the same conditions, the antiparallel triplex remains stable. (iv) Netropsin, a natural DNA minor groove-binding ligand, binds to the central site A4/T4of the duplex or triplex in an equimolar stoichiometry. Its association constant K is smaller for the parallel triplex ( approximately 1 x 10(7) M-1) than for the antiparallel one ( approximately 1 x 10(8) M-1). In contrast to the antiparallel structure, netropsin binding has no apparent effect on thermal stability of the parallel triple helix.     

Extreme stability of helices formed by water-soluble poly-N-substituted glycines (polypeptoids) with alpha-chiral side chains.

Poly-N-substituted glycines or "peptoids" are protease-stable peptide mimics. Although the peptoid backbone is achiral and lacks hydrogen-bond donors, substitution with alpha-chiral side chains can drive the formation of stable helices that give rise to intense CD spectra. To systematically study the solution properties and stability of water-soluble peptoid helices with alpha-chiral side chains, we have synthesized and characterized an amphipathic, 36-residue N-substituted glycine oligomer. CD was used to investigate effects of concentration and solvent environment on this helical peptoid. We saw no significant dependence of helical structure on concentration. Intense, "alpha-helix-like" CD spectra were observed for the 36-mer in aqueous, 2,2,2-trifluorethanol (TFE), and methanol solution, proving a relative insensitivity of peptoid helical structure to solvent environment. While CD spectra taken in these different solvents were fundamentally similar in shape, we did observe some interesting differences in the intensities of particular CD bands in the various solvents. For example, the addition of TFE to an aqueous solvent increases the degree of peptoid helicity, as is observed for polypeptide alpha-helices. Moreover, the helical structure of peptoids appears to be virtually unaffected by heat, even in an aqueous buffer containing 8 M urea. The extraordinary resistance of these peptoid helices to denaturation is consistent with a dominant role of steric forces in their structural stabilization. The structured polypeptoids studied here may have potential as robust mimics of helical polypeptides of therapeutic interest.     

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 β, ε, and ζ around the phosphate groups. However, the sugar pucker displays a more rich variation, resulting in conformations not usually associated with the canonical duplex structures. © 1995 John Wiley & Sons, Inc.     

Thermodynamic and computational studies of DNA triple helices containing a nucleotide or a non-nucleotide linker in the third strand.

In this paper we report a thermodynamic characterisation of stability and melting behaviour of four different triple helices at pH 6.0. The target duplex consists of 16 base pairs in alternate sequence of the type 5'-(purine)(m)(pyrimidine)(m)-3'. The four triplexes are formed by targeting the 16-mer duplex with an all pyrimidine 16-mer or 15-mer or 14-mer third strand. The 16-mer oligonucleotide contains a 3'-3' phosphodiester junction and corresponding triplex was named 16-mer P. The 14-mer oligonucleotide contains a non-nucleotide linker, the 1,2,3 propanetriol residue and the corresponding triplex was named 14-mer PT. For the 15-mer oligonucleotide both junctions were alternatively used and the relative triplexes were named 15-mer P and 15-mer PT, respectively. These linkers introduce the appropriate polarity inversion and let the third strand switch from one oligopurine strand of the duplex to the other. Thermal denaturation profiles indicate the initial loss of the third strand followed by the dissociation of the target duplex. Transition enthalpies, entropies and free energies were derived from differential scanning calorimetric measurements. The comparison of Gibbs energies reveals that a more stable triplex is obtained when in the third strand there is the lack of one nucleotide in the junction region and a propanetriol residue as linker was used. The thermodynamic data were discussed in light of molecular mechanics and dynamics calculations.     

NMR studies of DNA (R+)n.(Y-)n.(Y+)n triple helices in solution: imino and amino proton markers of T.A.T and C.G.C+ base-triple formation

High-resolution exchangeable proton two-dimensional NMR spectra have been recorded on 11-mer DNA triple helices containing one oligopurine (R)n and two oligopyrimidine (Y)n strands at acidic pH and elevated temperatures. Our two-dimensional nuclear Overhauser effect studies have focused on an 11-mer triplex where the third oligopyrimidine strand is parallel to the oligopurine strand. The observed distance connectivities establish that the third oligopyrimidine strand resides in the major groove with the triplex stabilized through formation of T.A.T and C.G.C+ base triples. The T.A.T base triple can be monitored by imino protons of the thymidines involved in Watson-Crick (13.65-14.25 ppm) and Hoogsteen (12.9-13.55 ppm) pairing, as well as the amino protons of adenosine (7.4-7.7 ppm). The amino protons of the protonated (8.5-10.0 ppm) and unprotonated (6.5-8.3 ppm) cytidines in the C.G.C+ base triple provide distinct markers as do the imino protons of the guanosine (12.6-13.3 ppm) and the protonated cytidine (14.5-16.0 ppm). The upfield chemical shift of the adenosine H8 protons (7.1-7.3 ppm) establishes that the oligopurine strand adopts an A-helical base stacking conformation in the 11-mer triplex. These results demonstrate that oligonucleotide triple helices can be readily monitored by NMR at the individual base-triple level with distinct markers differentiating between Watson-Crick and Hoogsteen pairing. Excellent exchangeable proton spectra have also been recorded for (R+)n.(Y-)n.(Y+)n 7-mer triple helices with the shorter length permitting spectra to be recorded at ambient temperature.(ABSTRACT TRUNCATED AT 250 WORDS)     

Crystal structure of an RNA duplex r(G GCGC CC)2 with non-adjacent G*U base pairs

The crystal structure of a self-complementary RNA duplex r(GGGCGCUCC)2with non-adjacent G*U and U*G wobble pairs separated by four Watson-Crick base pairs has been determined to 2.5 A resolution. Crystals belong to the space group R3; a = 33.09 A,alpha = 87.30 degrees with a pseudodyad related duplex in the asymmetric unit. The structure was refined to a final Rworkof 17.5% and Rfreeof 24.0%. The duplexes stack head-to-tail forming infinite columns with virtually no twist at the junction steps. The 3'-terminal cytosine nucleosides are disordered and there are no electron densities, but the 3' penultimate phosphates are observed. As expected, the wobble pairs are displaced with guanine towards the minor groove and uracil towards the major groove. The largest twist angles (37.70 and 40.57 degrees ) are at steps G1*C17/G2*U16 and U7*G11/C8*G10, while the smallest twist angles (28.24 and 27.27 degrees ) are at G2*U16/G3*C15 and C6*G12/U7*G11 and conform to the pseudo-dyad symmetry of the duplex. The molecule has two unequal kinks (17 and 11 degrees ) at the wobble sites and a third kink at the central G5 site which may be attributed to trans alpha (O5'-P), trans gamma (C4'-C5') backbone conformations. The 2'-hydroxyl groups in the minor groove form inter-column hydrogen bonding, either directly or through water molecules.