DNA structural features responsible for sequence-dependent binding geometries of Hoechst 33258

The complexes of Hoechst 33258 with poly[d(A-T)₂], poly[d(I-C)₂], poly[d(G-C)₂], and poly[d(G-m⁵C)₂] were studied using linear dichroism, CD, and fluorescence spectroscopies. The Hoechst-poly[d(I-C)₂] complex, in which there is no guanine amino group protruding in the minor groove, exhibits spectroscopic properties that are very similar to those of the Hoechst-poly[d(A-T)₂] complex. When bound to both of these polynucleotides, Hoechst exhibits an average orientation angle of near 45° relative to the DNA helix axis for the long-axis polarized low-energy transition, a relatively strong positive induced CD, and a strong increase in fluorescence intensity—leading us to conclude that this molecule also binds in the minor groove of poly[d(I-C)₂]. By contrast, when bound to poly[d(G-C)₂] and poly[d(G-m⁵C)₂], Hoechst shows a distinctively different behavior. The strongly negative reduced linear dichroism in the ligand absorption region is consistent with a model in which part of the Hoechst chromophore is intercalculated between DNA bases. From the low drug:base ratio onset of excitonic effects in the CD and fluorescence emission spectra, it is inferred that another part of the Hoechst molecule may sit in the major groove of poly[d(G-C)₂] and poly[d(G-m⁵C)₂] and preferentially stacks into dimers, though this tendency is strongly reduced for the latter polynucleotide. Based on these results, the importance of the interactions of Hoechst with the exocyclic amino group of guanine and the methyl group of cytosine in determining the binding modes are discussed. © 1996 John Wiley & Sons, Inc.     

On the interaction of daunomycin with synthetic alternating DNAs: sequence specificity and polyelectrolyte effects on the intercalation equilibrium

The interaction of daunomycin with ctDNA and six purine–pyrimidine alternating poly-deoxynucleotides has been studied using fluorometric and uv-visible absorption methods. In the explored binding range of r > 0.05, the intercalation of the drug into the DNAs proved to be anticooperative, as indicated by the pronounced upward curvature of all the Scatchard plots obtained. The experimental data have been analyzed according to the recent theory of Friedman and Manning, which describes the polyelectrolyte effects on the site binding equilibria, drug intercalation included. We found that, accounting for the polyelectrolyte effects in the neighbor site exclusion model, the experimental data were nearly equally well described, in a wide range of binding ratios, by assuming the presence of sequence specificity effects (site size = 2 base pairs, exclusion parameter n = 1) or its absence (site size = 1 base pair, n = 1.7). The relevant results are as follows: (a) Daunomycin binds to all the DNAs considered with a stoichiometry of approximately 1 drug for every two base pairs. (b) The anticooperative nature of the interaction is essentially polyelectrolytic in origin. (c) The binding affinity shown by the drug for the different sites considered decreases in the order of Gm⁵C > AT > AC-GT > IC > GC > AU, indicating a stabilizing effect of the —CH₃ group in position 5 of the pyrimidines. (d) The extent of quenching of the intrinsic fluorescence of daunomycin in the presence of DNA is bound to the presence, at the intercalation site, of a guanine residue, since GC, Gm⁵C, and AC-GT sites induce a nearly total quenching, whereas AT, AU, and IC sites act only partially in this respect. The structural results obtained from the daunomycin-d[(CGTACG)]₂ crystal suggest that the 2-NH₂ group of guanine might be responsible for such a phenomenon. The influence of both the temperature and the ionic strength on the free energy of drug intercalation into ctDNA, poly[d(G-C)] : poly[d(G-C)], and poly[d(A-C)] : poly[d(G-T)] is examined and discussed.     

Long-range allosteric effects on the B to Z equilibrium by daunomycin

Spectroscopic and fluorometric methods were used to study the binding of the anticancer drug daunomycin to poly[d(G-C)] and poly[d(G-m5C)] under a variety of solution conditions. Under high-salt conditions that favor the left-handed Z conformation, binding isotherms for the interaction of the drug with poly[d(G-C)] are sigmoidal, indicative of a cooperative binding process. Both the onset and extent of the cooperative binding are strongly dependent upon the ionic strength. The binding data may be explained by a model in which the drug preferentially binds to B-form DNA and acts as an allosteric effector on the B to Z equilibrium. At 2.4 M NaCl, binding of as little as one drug molecule per 20 base pairs (bp) results in the conversion of poly[d(G-C)] from the Z form entirely to the B form, as inferred from binding data and demonstrated directly by circular dichroism measurements. Similar results are obtained for poly[d(G-m5C)] in 50 mM NaCl and 1.25 mM MgCl2. Under these solution conditions, it is possible to demonstrate the Z to B structural transition in poly[d(G-m5C)] as a function of bound drug by the additional methods of sedimentation velocity and susceptibility to DNase I digestion. The transmission of allosteric effects over 20 bp is well beyond the range of the drug's binding site of 3 bp. Since daunomycin preferentially binds to alternating purine-pyrimidine sequences, which are the only sequences capable of the B to Z transition, the allosteric effects described here may be of importance toward understanding the mechanism by which the drug inhibits DNA replicative events.(ABSTRACT TRUNCATED AT 250 WORDS)     

Studies of the B‐Z transition of DNA: The temperature dependence of the free‐energy difference,the composition of the counterion sheath in mixed salt,and the preparation of a sample of the 5′‐d[T‐(m5C‐G)12‐T] duplex in pure B‐DNA or Z‐DNA form

It is often envisioned that cations might coordinate at specific sites of nucleic acids and play an important structural role, for instance in the transition between B‐DNA and Z‐DNA. However, nucleic acid models explicitly devoid of specific sites may also exhibit features previously considered as evidence for specific binding. Such is the case of the “composite cylinder” (or CC) model which spreads out localized features of DNA structure and charge by cylindrical averaging, while sustaining the main difference between the B and Z structures, namely the better immersion of the B‐DNA phosphodiester charges in the solution. Here, we analyze the non‐electrostatic component of the free‐energy difference between B‐DNA and Z‐DNA. We also compute the composition of the counterion sheath in a wide range of mixed‐salt solutions and of temperatures: in contrast with the large difference of composition between the B‐DNA and Z‐DNA forms, the temperature dependence of sheath composition, previously unknown, is very weak. In order to validate the model, the mixed‐salt predictions should be compared to experiment. We design a procedure for future measurements of the sheath composition based on Anomalous Small‐Angle X‐ray Scattering and complemented by ³¹P NMR. With due consideration for the kinetics of the B‐Z transition and for the capacity of generating at will the B or Z form in a single sample, the 5′‐d[T‐(m⁵C‐G)₁₂‐T] 26‐mer emerges as a most suitable oligonucleotide for this study. Finally, the application of the finite element method to the resolution of the Poisson‐Boltzmann equation is described in detail. © 2016 Wiley Periodicals, Inc. Biopolymers 105: 369–384, 2016.     

Divalent Cations are not Required for the Stability of the Low-Salt Z-DNA Conformation in Poly(dG-ethyl5 dC)

Abstract

It is demonstrated that poly(dG-ethyl⁵dC) adopts Z form in low-salt solution like poly(dGmethyl⁵dC). Its existence is, however, not contingent on the presence of divalent cations in the polynucleotide solution. The Z form is transformed into B form below room temperature. The arising B form cannot be transformed back into Z form by millimolar MgCl₂ concentrations. On the contrary, the addition of MgCl₂ at room temperature converts the low-salt Z form of poly(dG-ethyl⁵dC) into B form. It follows from the results that Z form is a stable DNA conformation not only at high but even at low ionic strengths.     

Evidence for DAPI intercalation in CG sites of DNA oligomer [d(CGACGTCG)]2: a 1H NMR study.

The interaction between 4',6-diamidino-2-phenylindole (DAPI) and the DNA oligomer [d(CGACGTCG)]2 has been investigated by proton one- and two-dimensional NMR spectroscopy in solution. Compared with the minor groove binding of the drug to [d(GCGATCGC)]2, previously studied by NMR spectroscopy, the interaction of DAPI with [d(CGACGTCG)]2 appears markedly different and gives results typical of a binding mechanism by intercalation. C:G imino proton signals of the [d(CGACGTCG)]2 oligomer as well as DAPI resonances appear strongly upfield shifted and sequential dipolar connectivities between cytosine and guanine residues show a clear decrease upon binding. Moreover, protons lying in both the minor and major grooves of the DNA double helix appear involved in the interaction, as evidenced principally by intermolecular drug-DNA NOEs. In particular, the results indicate the existence of two stereochemically non-equivalent intercalation binding sites located in the central and terminal adjacent C:G base pairs of the palindromic DNA sequence. Different lifetimes of the complexes were also observed for the two sites of binding. Moreover, due to the fast exchange on the NMR timescale between free and bound species, different interactions in dynamic equilibrium with the observed intercalative bindings were not excluded.     

DNA sequence dependent binding modes of 4',6-diamidino-2-phenylindole (DAPI)

The interactions of DAPI with natural DNA and synthetic polymers have been investigated by hydrodynamic, DNase I footprinting, spectroscopic, binding, and kinetic methods. Footprinting results at low ratios (compound to base pair) are similar for DAPI and distamycin. At high ratios, however, GC regions are blocked from enzyme cleavage by DAPI but not by distamycin. Both poly[d(G-C)]2 and poly[d(A-T)]2 induce hypochromism and shifts of the DAPI absorption band to longer wavelengths, but the effects are larger with the GC polymer. NMR shifts of DAPI protons in the presence of excess AT and GC polymers are significantly different, upfield for GC and mixed small shifts for AT. The dissociation rate constants and effects of salt concentration on the rate constants are also quite different for the AT and the GC polymer complexes. The DAPI dissociation rate constant is larger with the GC polymer but is less sensitive to changes in salt concentration than with the AT complex. Binding of DAPI to the GC polymer and to poly[d(A-C)].poly[d(G-T)] exhibits slight negative cooperativity, characteristic of a neighbor-exclusion binding mode. DAPI binding to the AT polymer is unusually strong and exhibits significant positive cooperativity. DAPI has very different effects on the bleomycin-catalyzed cleavage of the AT and GC polymers, a strong inhibition with the AT polymer but enhanced cleavage with the GC polymer. All of these results are consistent with two totally different DNA binding modes for DAPI in regions containing consecutive AT base pairs versus regions containing GC or mixed GC and AT base pair sequences. The binding mode at AT sites has characteristics which are similar to those of the distamycin-AT complex, and all results are consistent with a cooperative, very strong minor groove binding mode. In GC and mixed-sequence regions the results are very similar to those observed with classical intercalators such as ethidium and indicate that DAPI intercalates in DNA sequences which do not contain at least three consecutive AT base pairs.     

Shape readout of AT‐rich DNA by carbohydrates

Gene expression can be altered by small molecules that target DNA; sequence as well as shape selectivities are both extremely important for DNA recognition by intercalating and groove‐binding ligands. We have characterized a carbohydrate scaffold (1) exhibiting DNA “shape readout” properties. Thermodynamic studies with 1 and model duplex DNAs demonstrate the molecule's high affinity and selectivity towards B* form (continuous AT‐rich) DNA. Isothermal titration calorimetry (ITC), circular dichroism (CD) titration, ultraviolet (UV) thermal denaturation, and Differential Scanning Calorimetry were used to characterize the binding of 1 with a B* form AT‐rich DNA duplex d[5′‐G₂A₆T₆C₂‐3′]. The binding constant was determined using ITC at various temperatures, salt concentrations, and pH. ITC titrations were fit using a two‐binding site model. The first binding event was shown to have a 1:1 binding stoichiometry and was predominantly entropy‐driven with a binding constant of approximately 10⁸ M^?1. ITC‐derived binding enthalpies were used to obtain the binding‐induced change in heat capacity (ΔC_p) of ?225 ± 19 cal/mol·K. The ionic strength dependence of the binding constant indicated a significant electrolytic contribution in ligand:DNA binding, with approximately four to five ion pairs involved in binding. Ligand 1 displayed a significantly higher affinity towards AT‐tract DNA over sequences containing GC inserts, and binding experiments revealed the order of binding affinity for 1 with DNA duplexes: contiguous B* form AT‐rich DNA (d[5′‐G₂A₆T₆C₂‐3′]) >B form alternate AT‐rich DNA (d[5′‐G₂(AT)₆C_2‐3′]) > A form GC‐rich DNA (d[5′‐A₂G₆C₆T₂‐3′]), demonstrating the preference of ligand 1 for B* form DNA. © 2013 Wiley Periodicals, Inc. Biopolymers 101: 720–732, 2014.     

DNA-binding geometry dependent energy transfer from 4′,6-diamidino-2-phenylindole to cationic porphyrins

The circular and linear dichroism (CD and LD) spectral properties of the meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (TMPyP)–DNA complex at a [porphyrin]/[DNA] ratio below 0.015 showed that TMPyP intercalates between DNA base pairs. Contrarily, when cis–bis(N-methylpyridinium-4-yl)porphyrin (BMPyP) is associated with DNA, no CD spectrum was induced and a bisignate LD spectrum was observed. These spectral properties of both the TMPyP and BMPyP were essentially retained when the minor groove of the DNA was saturated with 4′,6-diamidino-2-phenylindole (DAPI). The fluorescence of the DNA-bound DAPI was effectively quenched by BMPyP and TMPyP. The quenching by BMPyP can be described through a pure static mechanism while TMPyP quenching produced an upward bending curve in the Stern–Volmer plot. Quenching efficiency was by far greater than predicted by the “sphere of action model”, suggesting that the DNA provides some additional processes for an effective energy transfer.     

Characterization of intermediate conformational states in the B↔Z transitions of poly(dG?dC) · poly(dG?dC)

Time-dependent uv absorption and CD spectrum changes in salt-induced conformational B → Z and Z → B transitions of poly(dG? dC) · poly(dG? dC) were measured. This polynucleotide does not convert directly from a right-handed double-helical B form to a left-handed double-helical Z form, but goes through an intermediate, B* form, with the B → B* transition proceeding nearly instantaneously, and then transforms gradually to the Z form. Uv absorption spectra of these B and B* forms are nearly identical, but their CD spectra are quite different. The CD spectrum of the B* form is identical with that obtained for DNA in high salt solutions and is similar to a spectrum which for some time was thought to be a C form. These B and B* forms have the same number of base pairs per turn [Sprecher, C.A., Baase, W.A. & Johnson, Jr., W.C. (1979) Biopolymers 18 , 1009–1019]. Kinetic measurements showed that uv absorption and CD intensities at fixed wavelengths do not change in a simple exponential curve. However, both the uv absorption spectrum change in the B → Z transition and the CD spectrum change in the B* → Z transition, respectively, have isosbestic points. In the B → Z transition, no hyperchromicity can be observed. These results suggest that this B* form unfolding or premelting process is a rate-determining step in the B* → Z transition and makes it easy for the unfolded or premelted polynucleotide to almost immediately fold into the Z form. The double helix does not dissociate into single strands and transforms from the B* form to the Z form point-by-point along the chain in a soliton-like manner of with a small amount of open states in which the bases are unpaired. Also, in the Z → B transition, the polynucleotide does not convert directly from the Z to the B form, but goes through a B*-like form. In this transition, the uv-absorption spectra also have an isosbestic point. The reaction velocity in the Z → B transition is much faster than that in the B → Z transition. Possibly, the positive CD band between 265 and 310 nm in the B form comes from a n-π* transition due to an interaction of the bases with sugarphosphate groups.     

N-2-acetylaminofluorene modification of poly(dG-m5dC)·poly(dG-m5dC) induces the Z-DNA conformation

Poly(dG-m⁵dC)·poly(dG-m⁵dC) was modified by treatment with N-acetoxy-N-2-acetylaminofluorene (N-Aco-AAF) and its conformation examined by circular dichroism (CD) and susceptibility to S₁ nuclease digestion. A sample with a modification level of 10% shows a CD spectrum characteristic of the Z form and is resistant to digestion by S₁ nuclease. The relative reactivity of several polymers with N-Aco-AAF was shown to follow the order of ease of formation of Z DNA: poly(dG-m⁵dC)·poly(dG-m⁵dC) > poly(dG-dC)·poly(dG-dC) > poly(dG)·poly(dC). This suggests that AAF reacts more readily with Z DNA than B DNA.     

Sequence and conformational effects on imino proton exchange in A.T- and A.U-containing DNA and RNA duplexes

¹H-nmr relaxation has been used to study the effect of sequence and conformation on imino proton exchange in adenine–thymine (A · T) and adenine–uracil (A · U) containing DNA and RNA duplexes. At low temperature, relaxation is caused by dipolar interactions between the imino and the adenine amino and AH2 protons, and at higher temperature, by exchange with the solvent protons. Although room temperature exchange rates vary between 3 and 12s^?1, the exchange activation energies (E_α) are insensitive to changes in the duplex sequence (alternating vs homopolymer duplexes), the conformation (B-form DNA vs A-form RNA), and the identity of the pyrimidine base (thymine vs uracil). The average value of the activation energy for the five duplexes studied, poly[d(A-T)], poly[d(A) · d(T)], poly[d(A-U)], Poly[d(A) · d(U)], and poly[r(A) · r(U)], was 16.8 ± 1.3 kcal/mol. In addition, we find that the average E_α for the A.T base pairs in a 43-base-pair restriction fragment is 16.4 ± 1.0 kcal/mol. This result is to be contrasted with the observation that the E_α of cytosine-containing duplexes depends on the sequence, conformation, and substituent groups on the purine and pyrimidine bases. Taken together, the data indicate that there is a common low-energy pathway for the escape of the thymine (uracil) imino protons from the double helix. The absolute values of the exchange rates in the simple sequence polymers are typically 3–10 times faster than in DNAs containing both A · T and G · C base pairs.     

Crystal and molecular structure of a DNA duplex containing the carcinogenic lesion O6-methylguanine

The crystal and molecular structure of the first DNA duplex containing the carcinogenic lesion O6MeG has been determined to a resolution of 1.9 A and refined to an R factor of 19%. (d[CGC-(O6Me)GCG])2 crystallizes in the left-handed Z DNA form and has crystal parameters and conformational features similar to those of the parent sequence [d(CG)3]2. The methyl groups on O6 of G4 and G10 have C5-C6-O6-O6Me torsion angles of 73 degrees and 56 degrees, respectively, and protrude onto the major groove surface. The base-pairing conformation for the methylated G.C base pairs is of the Watson-Crick type as opposed to a wobble-type conformation that had been proposed in a B DNA fragment. As in other Z DNA structures, a spine of hydration is seen in the minor groove.     

Interaction of Isoquinoline Alkaloids with Polymorphic DNA Structures

The interaction of berberine, palmatine, and coralyne with the B, Z, and H^L form of poly[d(G‐C)] was studied. Berberine and palmatine showed moderate binding to the B form, while coralyne showed higher binding, as revealed from spectroscopic and thermodynamic data. Berberine and coralyne binding to the B form was exothermic and enthalpy‐driven, while palmatine showed exothermic binding which was favored by both negative enthalpy and negative entropy changes. Berberine and palmatine neither bind nor converted the Z‐form structure to B form. Coralyne, on the other hand, exhibited a strong binding affinity to Z DNA structure that was enthalpy‐driven. Berberine binding to the H^L form was cooperative, exothermic, and favored by both negative enthalpy and negative entropy changes with the formation of an induced CD band. Palmatine showed weak binding, while coralyne showed a strong binding with the H^L form. The structural differences in the isoquinoline alkaloids appear to influence the affinity and mode of interactions with these polymorphic DNA structures.     

Effect of intercalative binding compared to external binding on Z/B equilibrium of poly d(GMe5C) using fluorescent oxazolopyridocarbazoles as probes

Using the fluorimetric determination of the binding isotherms in combination with circular dichroism, we have investigated the effect of the binding of the intercalating chromophore oxazolopyridocarbazole (OPC) to poly d(GMe5C) on B/Z equilibrium, compared to the effect of the external binder OPC derivative pentyl-2-OPC. The intercalating OPC appears to be very efficient in reversing left-handed poly d(GMe5C) into the right-handed conformation, according to a cooperative mode. For each OPC molecule intercalated into the B form, 7 base pairs were switched from the Z to B conformation. In contrast, the binding of the external binder pentyl-OPC resulted in a limited Z to B transition, involving the switch of 1.4 base pairs from the Z to B conformation. Moreover, OPC appears much more efficient than pentyl-OPC in inhibiting both the extent and kinetics of the salt-induced B/Z transition. At low drug to DNA ratio (D/P = 1/50), a 7-fold and 1.5-fold inhibition of the B/Z transition kinetics occurs in the presence of OPC and pentyl-OPC, respectively. These features are discussed in terms of the difference existing between the entropic contribution in the DNA binding of intercalating agents, compared to external binders.     

Interactions of polyamines with the DNA octamers d(m5CG)4 and d(GGAATTCC): A 1H‐NMR investigation

The interaction of two DNA octamers, d(m⁵CG)₄ and d(GGAATTCC), with the polyamines spermine⁴⁺ and spermidine³⁺, has been studied by means of ¹H‐nmr nuclear Overhauser effect (NOE) difference measurements. The experiments were performed at 10°C and for a polyamine charge to DNA charge (i.e., phosphate) ratio of 0.4, where the solution of d(m⁵CG)₄ contains about 50% Z‐form of the DNA. The results show that the polyamine intramolecular NOEs for the protons on the propyl chains are similarly negative with the two oligonucleotides, while those on the butyl chain show slightly more negative NOE with d(m⁵CG)₄ than with d(GGAATTCC). The fully N‐methylated analogues of spermine (Me₁₀Spn⁴⁺) and spermidine (Me₈Spd³⁺) as well as the diamines 1,3‐diaminopropane (DAP²⁺) and 1,4‐diaminobutane (putrescine²⁺) have been studied for the ability to transform d(m⁵CG)₄ from the B‐ to the Z‐form. ¹H‐nmr spectra showed the order spermine⁴⁺ > spermidine³⁺ > Me₁₀Spn⁴⁺ > Me₈Spd³⁺ > 1,3‐diaminopropane²⁺ > putrescine²⁺, with spermine showing the largest relative amount of Z‐DNA. ¹H‐nmr pulsed‐gradient self‐diffusion measurements of the triamines showed a large difference in the interaction of Spd and Me₈Spd with the two different duplexes. With the same duplex (either of the two), however, no difference between Spd and Me₈Spd can be seen. Within a two‐state model this is interpreted as a larger fraction of bound polyamines with d(m⁵CG)₄ than with d(GGAATTCC). © 1999 John Wiley & Sons, Inc. Biopoly 49: 41–53, 1999     

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.