Interactions of DNA with a new electron-deficient tentacle porphyrin: meso-Tetrakis[2,3,5,6-tetrafluoro-4-(2-trimethylammoniumethylamine)phenyl]porphyrin

A new electron-deficient tentacle porphyrin meso-tetrakis[2,3,5,6-tetrafluoro-4-(2-trimethylammoniumethylamine)phenyl]porphyrin (TθF₄TAP) has been synthesized. The binding interactions of TθF₄TAP with DNA polymers were studied for comparison to those of an electron-deficient tentacle porphyrin and an electron-rich tentacle porphyrin; these previously studied porphyrins bind to DNA primarily by intercalative and outside-binding modes, respectively. The three tentacle porphyrins have similar size and shape. The basicity of TθF₄TAP indicated that it has electronic characteristics similar to those of the intercalating electron-deficient tentacle porphyrin. However, TθF₄TAP binds to calf thymus DNA, [poly(dA-dT)]₂, and [poly(dG-dC)]₂ in a self-stacking, outside-binding manner under all conditions. Evidence for this binding mode included a significant hypochromicity of the Soret band, a conservative induced CD spectrum, and the absence of an increase in DNA solution viscosity. As found previously for the electron-rich porphyrin, the results suggest that combinations of closely related self-stacked forms coexist. The mix of forms depended on the DNA and the solution conditions. There are probably differences in the detailed features of the self-stacking adducts for the two types of tentacle porphyrins, especially at high R (ratio of porphyrin to DNA). At low R values, the induced CD signal of TθF₄TAP/CT DNA resembled that of TθF₄TAP/[poly(dA-dT)]₂, suggesting that TθF₄TAP binds preferentially at AT regions. Competitive binding experiments gave evidence that TθF₄TAP binds preferentially to [poly(dA-dT)]₂ over [poly(dG-dC)]₂. Thus, despite the long, positively charged, flexible substituents on the porphyrin, the binding of TθF₄TAP is significantly affected by base-pair composition. Similar characteristics were found previously for the electron-rich tentacle porphyrin. Thus, significant changes in electron richness have relatively minor effects on this outside binding selectivity for AT regions. TθF₄TAP is the first porphyrin with electron deficiency and shape similar to intercalating porphyrins that does not appear to intercalate. All porphyrins reported to intercalate have had pyridinium substituents. Thus, the electronic distribution in the porphyrin ring, not just the overall electron richness, may play a role in facilitating intercalation. © 1997 John Wiley & Sons, Inc. Biopoly 42: 203–217, 1997     

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.     

Characterization of the binding of YO to [poly(dA-dT)]2 and [poly(dG-dC)]2, and of the fluorescent properties of YO and YOYO complexed with the polynucleotides and double-stranded DNA

The interaction between the fluorescent dye YO (oxazole yellow) and the alternating polynucleotides [poly(dA-dT)]₂[the duplex of alternating poly(dA-dT)]and [poly(dG-dC)]₂[the duplex of alternating poly(dG-dC)] has been studied with optical spectroscopic techniques including absorbance, flow linear dichroism, CD, and fluorescence measurements. The principal features of the spectra are very similar for the two polynucleotide solutions, showing that YO binds quite similarly to AT and GC base pairs. From a strongly negative reduced linear dichroism (LD^r) in the dye absorption band, an induced negative CD, and transfer of energy from the bases to bound YO, we conclude that at low mixing ratios YO is intercalated in both [poly(dA-dT)]₂ and [poly(dG-dC)]₂. At higher mixing ratios an external binding mode starts to contribute, evidenced from the appearance of an exciton CD. The conclusion that YO binds in a similar way to AT and GC base pairs should be valid also for the dimer YOYO since its YO units have been found to bind to double-stranded (dsDNA) in the same way as the YO monomer. The fluorescence properties of YO and YOYO complexed with DNA or the polynucleotides have been characterized by studying the dependence of fluorescence intensity on temperature, mixing ratio, and ionic strength. The fluorescence intensity and fluorescence lifetime of YO-DNA decrease strongly with increasing mixing ratio, whereas the fluorescence intensity of YOYO-DNA shows a weaker dependence, indicating that the quantum yield depends on the distance between the YO chromophores on the DNA chain. Further, the fluorescence intensity of YO depends on the base sequence; the quantum yield and fluorescence lifetime for YO complexed with [poly(dG-dC)]₂ are about twice as large as for YO complexed with [poly(dA-dT)]₂. Measurements of excitation spectra at different mixing ratios and different emission wavelengths indicate that the fluorescence of the externally bound chromophores is negligible compared to the intercalated ones. © 1995 John Wiley & Sons, Inc.     

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).     

Synthesis, characterization and electrode adsorption studies of porphyrins coordinated to ruthenium(II) polypyridyl complexes

Two new porphyrins, meso-tris-3,4-dimethoxyphenyl-mono-(4-pyridyl)porphyrin (H₂MPy3,4DMPP) and meso-tris-3-methoxy-4-hydroxyphenyl-mono-(4-pyridyl)porphyrin (H₂MPy3M4HPP), and their ruthenium analogs obtained by coordination of [Ru(bpy)₂Cl]⁺ groups (where bpy = 2,2′-bipyridine) to the pyridyl nitrogens have been synthesized and studied by electronic absorption spectroscopy, cyclic voltammetry and spectroelectrochemistry. These ruthenated porphyrins couple Ru chromophores to porphyrins containing electroactive meso-substituents. The highest energy electronic absorption for the ruthenated complexes is assigned as a bpy(π) → bpy(π*) intraligand charge transfer while the next lowest energy electronic absorption is assigned as Ru(dπ) → bpy(π*) metal-to-ligand charge transfer (MLCT) transition. The Ru^III/II couples occur at approximately 0.95 V versus the SHE reference electrode in acetonitrile solutions. The first oxidation of the porphyrin is localized on the 3,4-dimethoxyphenyl and 3-methoxy-4-hydroxyphenyl substituents, respectively. Electroactive surfaces result from adsorption of these compounds onto glassy carbon electrodes followed by anodic cycling in acidic media.     

Interaction of water-soluble Cu(II), Ni(II), and Co(III) porphyrins with polynucleotides

The interaction of the Cu(II), Ni(II) and Co(III) complexes of the following six water-soluble cationic porphyrins with calf thymus DNA, poly(dG-dC)2 and poly(dA-dT)2 was studied by UV-visible and resonance Raman spectroscopy: tetrakis(2-N-) and (3-N-methylpyridyl) porphyrin (1, 2); monophenyl-tris(4-N-methylpyridyl)porphyrin (4); cis- and trans-diphenyl-bis (4-N-methylpyridyl)porphyrin (5, 6). The binding to nucleic acids was compared with that of tetrakis(4-N-methylpyridyl)porphyrin (3). If the N(+)-CH3 group is moved from the para (3) to the meta position (2), binding of the free porphyrin as well as that of the metal complexes is only gradually modified; thus, the square-planar Cu- and Ni-2 are intercalated at the G-C site whereas Co-2 is groove-bound at A-T. Additionally, Ni-2 is probably also intercalated at the A-T site. When the N(+)-CH3 group is located at ortho position (1), the high rotation barrier of the 2-N-methylpyridyl group prevents intercalation of Cu- and Ni-1, resulting in weak outside binding. At ionic strength mu = 0.2, there is no evidence of significant interaction of Co-1 with any of the polynucleotides. When the charged N-methylpyridyl groups in 3 are subsequently replaced by phenyl groups (4, 5/6), the tendency of the Cu(II) and Ni(II) complexes to bind to the outside of the helix or to intercalate only partially increases at the expense of full intercalation. The coulombic attraction remains strong, no significant differences can be detected between 3, 4, 5, and 6. Ni-4 binds to poly(dA-dT)2 in the same complicated manner as Ni-3. The outside-binding in Co-4, -5 and -6 differs slightly from that in Co-2 and Co-3.     

Vibrational and electronic circular dichroism study of the interactions of cationic porphyrins with (dG-dC)10 and (dA-dT)10

The interactions of two different porphyrins, without axial ligands-5,10,15,20-tetrakis(1-methylpyridinium-4-yl)porphyrin-Cu(II) tetrachloride (Cu(II)TMPyP) and with bulky meso substituents-5,10,15,20-tetrakis(N,N,N-trimethylanilinium-4-yl)porphyrin tetrachloride (TMAP), with (dG-dC)10 and (dA-dT)10 were studied by combination of vibrational circular dichroism (VCD) and electronic circular dichroism (ECD) spectroscopy at different [oligonucleotide]/[porphyrin] ratios, where [oligonucleotide] and [porphyrin] are the concentrations of oligonucleotide per base-pair and porphyrin, respectively. The combination of VCD and ECD spectroscopy enables us to identify the types of interactions, and to specify the sites of interactions: The intercalative binding mode of Cu(II)TMPyP with (dG-dC)(10), which has been well described, was characterized by a new VCD "marker" and it was shown that the interaction of Cu(II)TMPyP with (dA-dT)10 via external binding to the phosphate backbone and major groove binding caused transition from the B to the non-B conformer. TMAP interacted with the major groove of (dG-dC)10, was semi-intercalated into (dA-dT)10, and caused significant variation in the structure of both oligonucleotides at the higher concentration of porphyrin. The spectroscopic techniques used in this study revealed that porphyrin binding with AT sequences caused substantial variation of the DNA structure. It was shown that VCD spectroscopy is an effective tool for the conformational studies of nucleic acid-porphyrin complexes in solution.     

Porphyrin induced Z to B conversion of poly(dG-dC)2 in ethanol

The water soluble porphyrins H2TMpyP-2, H2TMpyP-4, and CuTMpyP-4 are found to bind to Z-form poly(dG-dC)2 in 60% ethanol (v/v) and to facilitate the conversion of the polymer to the B form. Metalloporphyrins with axial ligands (MnTMpyP-4, ZnTMpyP-4) interact to some degree with the Z form, but do not lead to extensive conversion to the B form. The conversion of the Z form into the B form was determined by CD titration experiments, which were used to quantitate the fraction of poly(dG-dC)2 present in each conformation. Under all conditions each bound porphyrin molecule converts multiple base pairs from Z to B. The kinetics of porphyrin reactions with Z-poly(dG-dC)2 in 60% ethanol were measured using two different detection techniques. Stopped flow spectrophotometry was used to observe the time-dependent spectral changes associated with the porphyrins during the reaction. Time-dependent changes in the poly(dG-dC)2 conformation were observed directly using CD. The porphyrin absorbance changes under the conditions of these experiments have a much shorter half time (t1/2 approximately 0.1 to 2 sec) than the CD changes (t1/2 approximately 10 sec). Thus it could be determined that a complex with spectral characteristics similar to those of the porphyrin intercalated into B-form poly(dG-dC)2 is produced while the polymer is predominantly in the Z form.     

A pared-down version of 5,10,15,20-tetra(N-methylpyridinium-4-yl)porphyrin intercalates into B-form DNA regardless of base composition: binding studies of tri(N-methylpyridinium-4-yl)porphyrins

Positively charged N-methylpyridinium-4-yl substituents promote the binding of a porphyrin to DNA, but they also impose steric constraints. To clarify when intercalative binding is most feasible, this report describes syntheses and binding studies of two tricationic ligands: 5,10,15-tri(N-methylpyridinium-4-yl)porphyrin (H2Tri4) and 5-methyl-10,15,20-tri(N-methylpyridinium-4-yl)porphyrin (H2MeTri4). Techniques used to characterize the binding interactions include viscometry and spectroscopic studies of the absorption, emission, and circular dichroism. The striking observation is that intercalation is the only detectable binding motif when the trisubstituted porphyrin H2Tri4 combines with [poly(dA-dT)]2, [poly(dG-dC)]2, or salmon testes DNA. H2Tri4 is, however, a limiting case. Parallel studies of H2MeTri4 and the copper(II) derivative Cu(MeTri4) reveal that external binding to [poly(dA-dT)]2 becomes important when a fourth meso substituent is present, even one as small as the methyl group. Intercalation of H2Tri4 is sterically feasible because two N-methylpyridinium-4-yl substituents can reside in the major groove, though the charge alignment is not optimal. However, the presence of the fourth substituent on H2MeTri4 further destabilizes the intercalated form, and external binding becomes competitive for a flexible host like [poly(dA-dT)]2.     

Antiviral Activity of Magnesium and Magnesium/poly r(A-U) Combinations Against two RNA Viruses

Abstract

Magnesium (Mg²⁺) potentiated the anti-vesicular stomatitis virus (VSV) activity of poly r(A-U) or poly r(G-C) and the anti-HIV-1 activity of poly r(A-U). Mg²⁺ did not affect the anti-VSV activity of poly (rI) ? poly (rC), poly (dA-dT) ? poly (dA-dT) or poly (dG-dC) ? poly (dG-dC). Modulation of one or more nuclear (nucleolar) processes of the host cell may be responsible for the synergistic antiviral activity.     

A series of meso-tris(N-methyl-pyridiniumyl)-(4-alkylamidophenyl) porphyrins: Synthesis,interaction with DNA and antibacterial activity

A series of meso-5,10,15-tris(N-methyl-4-pyridiniumyl)-20-(4-alkylamidophenyl) porphyrins were synthesized by derivatizing the amino group on the phenyl ring with the following hydrophobic groups: –C(O)C₇F₁₅, –C(O)CHCH₂, C(O)CH₃, –C(O)C₇H₁₅, and –C(O)C₁₅H₃₁. The cationic tris-pyridiumyl porphyrin core serves as a DNA binding motif and a photosensitizer to photomodify DNA molecules. The changes of the UV–Vis absorption spectra during the titration of these porphyrins with calf thymus DNA revealed a large bathochromic shift (up to 14 nm) and a hypochromicity (up to 55%) of the porphyrins Soret bands, usually considered as proof of porphyrin intercalation into DNA. Association constants (K) calculated according to the McGhee and von Hippel model, were in the range of 10⁶–10⁷ M⁻¹. An increase in hydrophobicity of the substituents at the 20−meso-position produced higher binding affinity. These porphyrins caused photomodification of the supercoiled plasmid DNA when a green laser beam at 532 nm was applied. Those with higher surface activity acted more efficiently as DNA photomodifiers. The porphyrin with a perfluorinated alkyl chain (–COC₇F₁₅) at the meso-20-position inhibited the growth of gram-positive bacteria (S. aureus, or S. epidermidis). Other porphyrins exhibited moderate activity against both gram-negative and gram-positive organisms.     

Quantitative analysis of DNA-porphyrin interactions

The binding of manganese(III)-tetra(4-N-methylpyridyl)porphyrin (MnTMpyP) with synthetic poly(dA-dT)2, poly(dI-dC)2, and poly(dG-dC)2 DNAs as well as calf thymus (CT) DNA has been quantitatively studied in detail using induced CD (circular dichroism) spectroscopy in the Soret absorption band. The CD spectra, which changed greatly depending on the porphyrin to DNA base-pair molar ratio (r), were normalized with respect to DNA concentration and deconvoluted. Three independent component binding modes (named mode 1, 2, and 3 in the order of increasing r values) were identified, which successfully simulated the observed CD spectra with negligibly small residuals for a wide range of r values. In the case of poly(dA-dT)2, poly (dI-dC)2, and CT DNA, all the three modes appeared, whereas in the case of poly(dG-dC)2 DNA, only modes 1 and 3 appeared in the r range studied. The r dependence of each binding mode, i.e., its relative affinity toward DNA, has been revealed by this analysis. Mode 1, which appeared as a single binding mode at very low r values (r < or = ca. 0.05), was inhibited by the addition of methyl green, a drug that preferentially binds to the major groove of poly (dA-dT)2 DNA. Berenil, a known minor groove binder to poly(dA-dT)2 or poly(dI-dC)2 DNA, inhibited modes 2 and 3. From these inhibition experiments as well as comparison of the component spectra for DNAs of different sequence, a binding site on DNA was proposed for each component binding mode. The number of DNA base pairs covered by a single molecule of porphyrin was estimated.     

Interactions of porphyrins with nucleic acids

The interactions of nucleic acids with water-soluble porphyrins and metalloporphyrins have been investigated by stopped-flow and temperature-jump techniques. Both natural DNA (calf thymus) and synthetic homopolymers [poly(dG-dC) and poly(dA-dT)] have been employed. The porphyrins studied belong to the tetrakis(4-N-methylpyridyl)porphine (H2TMpyP-4) series and can be divided into two groups: (i) those which have no axial ligands when bound to nucleic acids [e.g., Ni(II), Cu(II), and the nonmetallic derivatives] and (ii) those which maintain axial ligands upon binding [e.g., Mn(III), Fe(III), Co(III), and Zn(II) derivatives]. The reaction of both axially and nonaxially liganded porphyrins at AT sites is too rapid to be measured by the kinetic methods utilized, whereas at GC sites the interaction of the nonaxially liganded porphyrins is in the millisecond time range and can be monitored by both stopped-flow and temperature-jump techniques. These results corroborate previous static studies, utilizing visible spectroscopy and circular dichroism, which indicate that the formation of an intercalated complex occurs only at GC base pair sites with porphyrins which do not possess axial ligands. With all the porphyrins investigated, the complexes formed at AT sites are envisioned as being of an "external" type involving some degree of overlap between the porphyrin and the bases of the duplex. In relaxation experiments of poly-(dG-dC) with H2TMpyP-4, a large, reproducible effect is observed which can be analyzed as a single exponential. Rate constants for association and dissociation of the H2TMpyP-4/poly(dG-dC) complex are 3.7 X 10(5) M-1 s-1 and 1.8 s-1, respectively. Relaxation studies of mixtures of poly(dA-dT) and poly(dG-dC) with H2TMpyP-4 indicate that the transfer of the porphyrin from one homopolymer to another occurs via a mechanism involving dissociation rather than direct transfer.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fluorescence decay of ethidium bromide in the presence of the Z-conformation of poly(dG-dC) and of poly(dG-dC) modified by chlorodiethylenetriamine platinum(II) chloride

A time-resolved fluorescence study of ethidium bromide (EB) in the presence of poly(dG-dC) and of poly(dG-dC) modified by chlorodiethylenetriamine platinum(II) chloride is presented under solvent conditions in which these polymers adopt the Z-conformation (high ionic strength). It is shown that these polynucleotides can intercalate a very small quantity of EB. The binding parameters have been determined. The fluorescence lifetime of EB is slightly higher when bound to the Z-conformation (?25 ns) than when bound to the B-conformation (?23.7 ns). The nature of the salt has been checked. In the presence of 2.5M NaClO₄, no transition from the Z-conformation to another conformation is observed when EB is added. On the contrary, in the presence of 4.25M NaCl, EB induces a cooperative transition from the Z-conformation to a conformation characterized by a much higher affinity for EB intercalation. In the case of poly(dG-dC) this last conformation is identical to the one observed at low ionic strength (B-conformation), but in the case of the platinated polymer this conformation is slightly different, as judged by the smaller value of the fluorescence lifetime of the intercalated EB.     

The CD of ligand-DNA systems. 2. Poly(dA-dT) B-DNA.

A systematic theoretical study of the CD of [poly(dA-dT)]2 and its complexes with achiral small molecules is presented. The CD spectra of [poly(dA-dT)]2 and of poly(dA):poly(dT) are calculated for various DNA structures using the matrix method. The calculated and experimental spectra agree reasonably well for [poly(dA-dT)]2 but less well for poly(dA):poly(dT). The calculated CD spectrum of [poly(dA-dT)]2 fails to reproduce the wavelength region of 205-245 nm of the experimental spectrum. This discrepancy can be explained by a magnetic dipole allowed transition contributing significantly to the CD spectrum in this region. The induced CD of a transition moment of a molecule bound to [poly(dA-dT)]2 is also calculated. As was the case for [poly(dG-dC)]2, the induced CD of a groove bound molecule is one order of magnitude stronger than that of an intercalated molecule. The calculations also show considerable differences between pyrimidine-purine sites and purine-pyrimidine sites. Both signs and magnitudes of the CD induced into ligands bound in the minor groove agree with experimental observations.     

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.     

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.     

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.     

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).     

Studies on synthetic chromatins containing poly(dA-dT)·poly(dA-dT) and poly(dG-dC)·poly(dG-dC)

Core histones, (H2A,H2B,H3,H4)₂, were reconstituted with the synthethic polynucleotides poly(dA-dT)·poly(dA-dT) and poly(dG-dC)·poly(dG-dC) to yield synthetic chromatins containing 200 basepairs per octamer. These synthetic chromatins displayed a 36% decrease in the circular dichroism (CD) peak ellipticity from the value of the polynucleotide free in solution; the poly(dA-dT)·poly(dA-dT)/chromatin showed an increase in the complexity of the thermal denaturation profile compared to that of the polynucleotide. Both the temperature of maximum $\text{d}\text{h}\text{d}\text{T}$ for each transition (T_m) and the relative amount of poly(dA-dT)·poly(dA-dT) in the synthetic chromatin melting in each of the four thermal transitions is a function of the ionic strength over the 0–5 mM sodium phosphate range (0.25 mM EDTA, pH 7.0); a shift of material toward higher melting transitions was observed with increasing ionic strength. The CD peak ellipticity value for both synthetic chromatins was ionic strength-independent over the 0–5 mM sodium phosphate range. These results are in contrast to those observed with $\text{H}\text{1}\text{H}\text{5}$ stripped chicken erythrocyte chromatin (Fulmer, A. and Fasman, G.D. (1979) Biopolymers 18, 2875–2891), where an ionic strength dependence was found. Differences in the CD spectra between poly(dA-dT)·poly(dA-dT)/chromatin, poly(dG-dC)·poly(dG-dC)/chromatin and $\text{H}\text{1}\text{H}\text{5}$ stripped chicken erythrocyte chromatin suggest subtle differences in assembly. Finally, the temperature dependence of the CD spectra of poly(dA-dT)·poly(dA-dT)-containing synthetic chromatin, which is similar to that for the polynucleotide, suggests the core histone bound polynucleotide has a large degree of conformational flexibility allowing it to undergo the premelt transition.