Raman spectroscopic elucidation of DNA backbone conformations for poly(dG-dT).poly(dA-dC) and poly(dA-dT).poly(dA-dT) in CsF solution

Raman spectra have been recorded for poly(dG-dT) · poly(dA-dC) and poly(dA-dT) · poly(dA-dT) in low salt and at high concentrations of CsF. Poly(dG-dT) · poly(dA-dC) shows no change in the 682-cm^?1 guanine mode, demonstrating the absence of the Z-structure at high salt. The 790-cm^?1 phosphodiester symmetric stretch, however, shifts up 5 cm^?1 in 4.3M CsF, suggesting a slight conformational change, associated with ion binding or hydration changes. Poly(dA-dT) · poly(dA-dT) shows an additional broad band at 816 cm^?1, attributed to the phosphodiester modes associated with the C3′-endo deoxyribose units in the alternating B-structure. In this case, both the 841- and the 816-cm^?1 asymmetric phosphodiester stretches, associated with the C2′- and C3′-endo units, shift down on addition of CsF in a sequential manner. Correlation of this sequence with that previously observed for the two ³¹P-nmr resonances, establishes that the phosphodiester stretching frequencies depend on the conformation of the 5′-sugar, and not on the 3′-sugar.     

Biphasic helix–coil transition of the ethidium bromide·poly(dA-dT) and the propidium diiodide·poly(dA-dT) Complexes. Stabilization of base-pair regions centered about the intercalation site

The nonexchangeable base and sugar proton nmr resonances and the 260 and 278-nm uv-absorbance bands of the nucleic acid were utilized to monitor the temperature-dependent duplex-to-strand transition of the alternating purine–pyrimidine deoxyribopolynucleotide poly(dA-dT) in the absence and presence of ethidium bromide (EB) at phosphate/drug = 50, 28, and 15 and propidium diiodide (PI) at P/D = 50, 25, 15, 10, and 5 in 0.1 M salt between 50° and 100°C. The nmr and optical methods monitor a biphasic duplex-to strand transition for the drug–poly(dA-dT) complexes. We have monitored the dissociation of the drug from the complex at the ethidium bromide phenanthridine ring and side-chain proton nmr resonances and the propidium diiodide 494 and 535-nm uv-absorbance bands and demonstrate that dissociation of the drug corresponds to the higher temperature transition in the biphasic nucleic acid melting curves. The lower temperature cooperative transition is assigned to the opening of drug-free AT base-pair regions in the drug–poly(dA-dT) complex and exhibits an increase in transition midpoint and a decrease in cooperativity with increasing drug concentration. The higher temperature cooperative transition is assigned to the opening of AT base-pair regions centered about the bound drug in the complex and exhibits an increase in the transition midpoint on raising the drug concentration. The large upfield shifts of the phenanthridine ring (but not side chain) protons of ethidium bromide on complex formation demonstrate intercalation of the drug between base pairs of the poly(dA-dT) duplex. The nucleic acid base and sugar resonances of poly(dA-dT) in 0.1 M phosphate undergo chemical shift changes between 0° and 50°C indicative of premelting conformational transition(s).     

Binding of tetrakis(pyrazoliumyl)porphyrin and its copper(II) and zinc(II) complexes to poly(dG-dC)2 and poly(dA-dT)2

Interactions of cationic porphyrins bearing five-membered rings at the meso position, meso-tetrakis(1,2-dimethylpyrazolium-4-yl)porphyrin (MPzP; M is H₂, Cu^II or Zn^II), with synthetic polynucleotides poly(dG-dC)₂ and poly(dA-dT)₂ have been characterized by viscometric, visible absorption, circular dichroisim and magnetic circular dichroism spectroscopic and melting temperature measurements. Both H₂PzP and CuPzP are intercalated into poly(dG-dC)₂ and are outside-bound to the major groove of poly(dA-dT)₂, while ZnPzP is outside-bound to the minor groove of poly(dA-dT)₂ and surprisingly is intercalated into poly(dG-dC)₂. The binding constants of the porphyrin and poly(dG-dC)₂ and poly(dA-dT)₂ are on the order of 10⁶ M⁻¹ and are comparable to those of other cationic porphyrins so far reported. The process of the binding of the porphyrin to poly(dG-dC)₂ and poly(dA-dT)₂ is exothermic and enthalpically driven for H₂PzP, whereas it is endothermic and entropically driven for CuPzP and ZnPzP. These results have revealed that the kind of the central metal ion of metalloporphyrins influences the characteristics of the binding of the porphyrins to DNA.Electronic Supplementary Material Supplementary material is available for this article at and is accessible for authorized users.     

Conformation of poly(dG-dC)·Poly(dG-dC) and Poly(dA-dT)·Poly(dA-dT) interacting with the antitumor drug cis-[Pt(NH32]Cl2

The interaction of cis-dichlorodiammine platinum(II) with poly(dG-dC)·poly(dG-dC) and poly(dA-dT) ·poly(dA-dT) was studied by circular dichroism. Significant conformational changes were induced in both alternating polymers: in the case of poly(dG-dC) ·poly(dG-dC) the spectra were not conclusive in terms of a well defined conformation, even if the presence of left-handed helices could be suggested. For poly(dA-dT)·poly(dA-dT) the data were interpreted in terms of a dimer-helix → single hairpin helix transition induced by the metal. The results obtained are discussed with reference to the antitumor activity of the drug.     

Comparison of the helix–coil conformational changes of poly(deoxyadenylate-deoxytymidylate) and poly(deoxyadenylate-deoxythymidylate) induced by variations of hydrogen-ion concentration

Double-helical poly(dG-dC) and poly(dA-dT) are DNA analogs in which the interactions between the two strands of the helix are, respectively, either the stronger G/C type or the weaker A/T type along the entire length of macromolecules. Thus, these synthetic polynucleotides can be considered as representatives of the most stable and the least stable DNA. In the investigations presented here, potentiometric titrations and stopped-flow kinetic experiments were carried out in order to compare the pH-induced helix–coil conformations (10°C and 150mM [Na⁺]) the pH of the helix–coil transition (pH_m) is 12.81 for poly(dG-dC) and 11.76 for poly(dA-dT). The unwinding of double-helical poly(dG-dC) initiated by a sudden change in pH was found to be a simple exponential process with rate constants in the range of 200–600 sec^?1, depending on the final value of the pH jump. The intramolecular double-helix formation of poly(dG-dC) was studied by lowering the pH of the solutions from a value above pH_m to that below pH_m in dilute solutions (15.5 ug/ml [polymer]). Under these conditions, the observed rewinding reactions displayed a major and two exponential phases, all of which were independent of polymer concentration. From the comparison of the results of poly(dA-dT) and poly(dG-dT) would unwind faster than poly(dG-dC). However, if the pH jumps are such that they present the same perturbation of these polymers relative to their pH_m values, no significant differences exist between the rates of helix–coil conformation changes of poly(dA-dT) and poly(dG-dC).     

Fractionation of poly (dA-dT) by gel chromatography

A commercial sample of poly (dA-dT), a copolymer of 2′-deoxyribosyladenosine (dA) and 2′-deoxyribosylthymidine (dT) of perfectly alternating sequence, was fractionated by chromatography on Agarose gel. Paucidisperse fractions of different molecular size were obtained. The plot of log s⁰_20,w values shows a linear dependence on V_e. The buoyant densities of individual fractions do not differ over the molecular size range studied. On the other hand, the heat-induced hyperchromic effect was found to depend on molecular size below a certain limit, s⁰_20,w = 4.12 S.     

Conformational transitions of poly(dA-dT)poly(dA-dT) in ethanolic solutions.

Examination of circular dichroic and phosphorus nuclear magnetic resonance spectra showed that poly(dA-dT)-poly(dA-dT) exhibited an ethanol-induced transition to the A form in an Na+ containing medium like natural DNAs. A mere replacement of the Na+ by Cs+ counterions meant that the polynucleotide was with a little cooperativity transformed into a novel conformation displaying a deep negative band in the long wavelength part of the CD spectrum. The presence of very low concentration of Cs2+ shifted the midpoint of the transition to a lower content of ethanol.     

Strance double helix of poly(dA-dT) in high-salt solution

³¹P and ¹H NMR studies indicate that double stranded poly(dA-dT) adopts an unusual structure in high-CsF solution, in which the dA residues occur in a unique geometry. This structure is different from the high-salt form of poly(dG-dC).     

Titration of poly(dA-dT) . poly(dA-dT) in solution at variable NaCl concentration

CD and uv absorption data showed that high molecular weight poly(dA-dT) . poly(dA-dT), at 298 K, undergoes an acid-induced transition from B-double helix to random coil in NaCl solutions of different concentrations, ranging from 0.005 to 0.600M. Similarly, titration of the polynucleotide with a strong base causes duplex-to-single strands transition. The base- and acid-induced transitions were both reversible by back-titration (with an acid or, respectively, with a base): the apparent pKa were the same in both directions. However, the number of protons per titratable site (adenine N1) required to reach half-denaturation was in great excess over the stoichiometric value; to a much larger extent, the same effect was observed also for the deprotonation of the N3H sites of thymine. Moreover, in the basic denaturation experiments, at low salt concentrations ([NaCl]< or =0.300M) less acid than calculated was needed to back-titrate the base excess to half-denaturation. Both effects could be qualitatively justified on the basis of the counterion condensation theory of polyelectrolytes and considering the energy barrier created by the negatively charged phosphodiester groups to the penetration of the OH- ions inside the double helix and the screening effect of the Na+ ions on such charges, in the deprotonation experiments.     

Conformational variability of poly(dA-dT).poly(dA-dT) and some other deoxyribonucleic acids includes a novel type of double helix

The article reviews data indicating that poly(dA-dT).poly(dA-dT) is able of adopting three distinct double helical structures in solution, of which only the A form conforms to classical notions. The other two structures have dinucleotides as double helical repeats. At low salt concentrations poly(dA-dT).poly(dA-dT) adopts a B-type alternating conformation which is exceptionally variable. Its architecture can gradually move in the limits demarcated by the CD spectra with inverted long wavelength CD bands and the 31P NMR spectra with a very low and a 0.6 ppm separation of two resonances. Contrary to Z-DNA, the 31P NMR spectrum of the limiting alternating B conformation of poly(dA-dT).poly(dA-dT) is characterized by an upfield shift of one resonance. We attribute the exceptional conformational flexibility of the alternating B conformation to the unequal tendency of bases in the dA-dT and dT-dA steps to stack. However, by assuming the limiting alternating B conformation, the variability of the synthetic DNA is not exhausted. Specific agents make it isomerize into another conformation by a fast, two-state mechanism, which is reflected by a further deepening of the negative long wavelength CD band and a downfield shift of the 31P NMR resonance of poly(dA-dT).poly(dA-dT) that was constant in the course of the gradual alterations of the alternating B conformation. These changes are, however, qualitatively different from the way poly(dG-dC).poly(dG-dC) behaves in the course of the B-Z isomerization. Poly(dG-dC).poly(dG-dC) displays purine-pyrimidine (dGpdC) resonance in the characteristic downfield position, while the downfield resonance of poly(dA-dT).poly(dA-dT) belongs to the pyrimidine-purine (dTpdA) phosphodiester linkages. Consequently, phosphodiester linkages in the purine-pyrimidine steps play a similar role in the appearance of the Z form to the pyrimidine-purine phosphodiesters in the course of the isomerization of poly(dA-dT).poly(dA-dT). This excludes that the high-salt structures of poly(dA-dT).poly(dA-dT) and poly(dG-dC).poly(dG-dC) are members of the same conformational family. We call the high-salt conformation of poly(dA-dT).poly(dA-dT) X-DNA. It furthermore follows from the review that synthetic molecules of DNA with alternating purine-pyrimidine sequences of bases can adopt either the Z form or the X form, or even both, depending on the environmental conditions. This introduces a new dimension into the DNA double helix conformational variability. The possible biological relevance of the X form is suggested by experiments with linear molecules of natural DNA.(ABSTRACT TRUNCATED AT 400 WORDS)     

B-X transition in synthetic and natural (dA-dT)n.(dA-dT)n sequences

AB-X transition of polyh(dA-dT).poly(dA-dT) was observed to occur in methanol-water mixtures with methanol concentrations higher than 50% in the presence of a specific combination of monovalent and divalent cations. In the presence of Na+, divalent cations induce denaturation of poly(dA-dT).poly(dA-dT) accompanied by condensation and/or aggregation, and effect similar to that observed previously with random sequence DNA (Votavová, Kucerová, Felsberg and Sponar, J. Biomol. Struct. Dyn. 4,477-489, 1986). In the presence of Cs+ cations a B-X transition was induced by addition of Ca2+ or Mn2+ but not Mg2+ or Ni2+ ions. Circular dichroism and ultraviolet spectroscopy demonstrate that the X conformation is a double stranded form of poly(dA-dT).poly(dA-dT) belonging presumably to the B family which, however has an altered base stacking. The X conformation of poly(dA-dT).poly(dA-dT) found in methanol-water mixtures is a condensed and/or aggregated form. In contrast, the X conformation characterized by similar CD spectra observed in high salt concentrations is not aggregated up to a concentration of 6 M CsF. In methanol-water mixtures (A+T)-rich bacterial DNA behaves essentially as a random sequence DNA revealing no detectable amount of the X form. On the other hand crab (Cancer pagurus) satellite and crab non-satellite DNAs containing varying amounts of (dA-dT)n.(dA-dT)n sequences were shown to undergo a B-X transition, at least partly, in both methanol-water mixtures and 6 M CsF solutions.     

A kinetic analysis of cyanine selectivity: CCyan2 and Cyan40 intercalation into poly(dA-dT) x poly(dA-dT) and poly(dG-dC) x poly(dG-dC)

A T-jump investigation of the binding of Cyan40 [3-methyl-2-(1,2,6-trimethyl-4(1H)pyridinylidenmethyl)-benzothiazolium ion] and CCyan2 [3-methyl-2-[2-methyl-3-(3-methyl-2(3H)-benzothiazolylidene)-1-propenyl]-benzothiazolium ion] with poly(dA-dT) x poly(dA-dT) and poly(dG-dC) x poly(dG-dC) is performed at I = 0.1M (NaCl), 25 degrees C and pH 7. Two kinetic effects are observed for both systems. The binding process is discussed in terms of the sequence D + P <==> P,D <==> PD(I) <==> PD(II), which leads first to fast formation of a precursor complex P,D and then to a partially intercalated complex PD(I) which converts to the fully intercalate complex PD(II). Concerning CCyan2 the rate parameters depend on the polymer nature and their analysis shows that in the case of poly(dG-dC) x poly(dG-dC) the most stable bound form is the fully intercalated complex PD(II), whereas in the case of poly(dA-dT) x poly(dA-dT) the partially intercalated complex PD(I) is the most stable species. Concerning Cyan40, the rate parameters remain unchanged on going from A-T to G-C indicating that this dye is unselective.     

Conformational Isomerizations of the Poly(dA-dT) and Poly(amino2dA-dT) Duplexes Involving the Unusual X-DNA Double Helix: A Fourth Derivative Spectrophotometric Study

Abstract

Fourth derivative spectrophotometry has been applied to monitor conformational isomerizations of polynucleotides for the first time. The transitions studied have been the B-A and A-X isomerizations of poly(dA-dT) and the B-X one of poly(amino²dA-dT). Parameters obtained from the fourth derivative spectra have been used to follow these conformational changes. The A form of poly(dA-dT) has been characterized by a new fourth derivative peak at 293.0 nm which can be associated to interstrand adenine-adenine interactions. Furthermore, some of the fourth derivative peaks in the long wavelength region (270–310 nm) can be related to stacking interactions present in the polynucleotide double helices. The tentative assignment of these peaks, particularly that at 299.0 nm in the derivative spectra of poly(amino²dA-dT), to n→π^* electronic transitions is discussed.     

Mutagen–nucleic acid complexes at the polynucleotide duplex level in solution: Intercalation of proflavine into poly(dA-dT) and the melting transition of the complex

The nmr chemical shifts and line widths of the nucleic acid base and sugar proton resonances and the proflavine ring protons can be monitored through the melting transition of the proflavine + poly(dA-dT) complex, phosphate/dye (P/D) ratio = 24 and 8 in 1M salt solution. The nucleic acid and mutagen protons in the complex are in fast exchange between duplex and strand states with the midpoint of the melting transition monitored at the nucleic acid resonances increasing from 72.6°C for poly(dA-dT) to 78.1°C for the P/D = 24 complex and 83.4°C for the P/D = 8 complex in 1M salt solution. The melting transition monitored by the proflavine resonances were 80.0°C for the P/D = 24 complex and 84.3°C for the P/D = 8 complex in 1M salt solution. Since the nucleic acid is in excess at high P/D ratios, the nucleic acid transitions are an average for the opening of mutagen-free and mutagen-bound base-pair regions, while the proflavine transitions monitor the melting of mutagen-bound base-pair regions. The observed 0.75 to 0.95 ppm unfield shift at all four proflavine protons on formation of the complex with poly(dA-dT) provides direct evidence for intercalation of the mutagen between base pairs of the nucleic acid duplex. We have deduced the approximate overlap geometry between the proflavine ring and nearest-neighbor base pairs at the intercalation site from a comparison between experimental proflavine complexation shifts and those calculated for various stacking orientations. The experimental chemical shift of the poly(dA-dT) adenine H-2 resonance in the duplex state in the absence and presence of proflavine suggests that intercalation occurs preferentially at dT-dA sites. The selective chemical shift changes at the sugar H-2′,2″ and H-3′ resonances of the poly(dA-dT) duplex on complex formation demonstrates changes in the sugar pucker and/or torsion angles of the sugar phosphate backbone at the intercalation site.     

Spectrophotometric and NMR analysis of the interaction of fluorinated mono- and bifunctional intercalators with DNA, poly(dA-dT), and poly(dG-dC)

We have synthesized and investigated the DNA binding properties of three fluorinated acridine derivatives—a monomer (I), a short dimer (II) and a long dimer (III). Only III has a sufficiently long chain bridging the two acridine nuclei to permit binding by bisintercalation. Analysis of the equilibrium and kinetic binding properties of these compounds to poly(dA-dT) demonstrates that they behave very similarly to their unfluorinated parent compounds. Helix extension, as determined by viscosity measurements, shows that both compounds I and II bind by monointercalation while III binds by bisintercalation. These results are confirmed by ¹⁹F-nmr analysis, which indicates, in particular, that the two chromophores of III share the same molecular environment as that of I in the presence of either calf thymus DNA or poly(dA-dT). Negative nuclear Overhauser effects in the presence of DNA indicate tight binding such that the motion of the ligands is governed by the polynucleotide dynamics. Optical titrations establish that in 4M NaCl, both I and III bind to calf thymus DNA, but no binding was observed with poly(dG-dC). This result is in contrast to those for dimers of ethidium, which show substantial binding to polynucleotides under high salt conditions. Nuclear magnetic resonance experiments, however, carried out at considerably higher concentrations, show that compound I does indeed bind to poly(dG-dC) under these high salt conditions, albeit weakly, and leads to a conversion of the polynucleotide from a left-handed to a right-handed conformation.     

UV Light-Induced Crosslinking of the Strands of Poly(dA-dT) and Related Alternating Purine-Pyrimidine DNAs

Abstract

Alkaline agarose gel electrophoresis was used to detect UV-induced crosslinking of the strands of poly(dA-dT) and related alternating purine-pyrimidine DNAs in solutions stabilizing various polynucleotide conformations. Strands of the B-form and A-form of poly(dA-dT) were not crosslinked but a UV dose-dependent retarded species appeared in the denaturing gels in parallel with the polynucleotide isomerization into the unusual X-form. Most other polynucleotides adopting the X-form were crosslinked as well. The exceptions include the X-forms of poly(dA-butyl⁵dU) and poly(dA-pentyl⁵dU) whose strands do not crosslink because the long exocyclic substituents attached to uracil make the photodimerization impossible. Strands of poly (amino²dA-dT) and poly(dA, amino ²dA-dT), the latter polynucleotide containing roughly equal amounts of amino ²adenine and adenine, also do not crosslink upon UV irradiation because they isomerize into an A-like conformation which is different from the X- form of poly (dA-dT). In contrast, strands of the mixed copolymers of poly(dA, amino ²dA-dT) containing low amino ²adenine contents are crosslinked upon UV irradiation, in accordance with the observation that they isomerize into the X-form.     

NMR relaxation and the structure of a synthetic DNA poly(dA-dT).poly(dA-dT)

1H-1H and 31P-1H nuclear Overhauser effects and 31P NMR spin-lattice relaxation times were measured for a synthetic DNA poly(dA-dT).poly(dA-dT) in a low-salt aqueous solution. The results have shown that all bases in the double helix are anti-orientated with respect to deoxyribose residues and that the sugar-phosphate backbone has an alternating architecture.     

Protonated polynucleotide structures. IX. Disproportionation of poly (G)-poly (C) in acid medium

The interaction between poly (G) and poly (C) was investigated in neutral and acid medium by optical methods. Three main points arise from this investigation. (1) The formation of poly (G)·poly (C) was complete only above an ionic strength of about 0.6M [Na⁺]. Lowering the ionic strength increased the amounts of free poly (G) and free poly (C) that could be detected. (2) When titrating towards acid pH values a transition took place which was characterized by potentiometry, mixing curves, and circular dichroism: a three-stranded poly (G)·poly (C)·poly (C⁺) complex was formed analogous to the transition observed for the acid titration of poly (I)·poly (C). (3) Even when the poly (G)·poly (C) complex was incompletely formed (at low ionic strength) in neutral medium all poly (C) entered the triple-stranded complex.