Mixed Mode of Ligand-DNA Binding Results in S-Shaped Binding Curves

Abstract

S-shaped binding curves often characterize interactions of ligands with nucleic acid molecules as analyzed by different physicochemical and biophysical techniques. S-shaped experimental binding curves are usually interpreted as indicative of the positive cooperative interactions between the bound ligand molecules. This paper demonstrates that S-shaped binding curves may occur as a result of the “mixed mode” of DNA binding by the same ligand molecule. Mixed mode of the ligand-DNA binding can occur, for example, due to 1) isomerization or dimerization of the ligands in solution or on the DNA lattice, 2) their ability to intercalate the DNA and to bind it within the minor groove in different orientations. DNA- ligand complexes are characterized by the length of the ligand binding site on the DNA lattice (so-called “multiple-contact” model). We show here that if two or more complexes with different lengths of the ligand binding sites could be produced by the same ligand, the dependence of the concentration of the complex with the shorter length of binding site on the total concentration of ligand should be S-shaped. Our theoretical model is confirmed by comparison of the calculated and experimental CD binding curves for bis-netropsin binding to poly(dA-dT) poly(dA-dT). Bis-netropsin forms two types of DNA complexes due to its ability to interact with the DNA as monomers and trimers. Experimental S-shaped bis-netropsin-DNA binding curve is shown to be in good correlation with those calculated on the basis of our theoretical model. The present work provides new insight into the analysis of ligand-DNA binding curves.     

Mixed mode of ligand-DNA binding results in S-shaped binding curves

S-shaped binding curves often characterize interactions of ligands with nucleic acid molecules as analyzed by different physico-chemical and biophysical techniques. S-shaped experimental binding curves are usually interpreted as indicative of the positive cooperative interactions between the bound ligand molecules. This paper demonstrates that S-shaped binding curves may occur as a result of the "mixed mode" of DNA binding by the same ligand molecule. Mixed mode of the ligand-DNA binding can occur, for example, due to 1) isomerization or dimerization of the ligands in solution or on the DNA lattice, 2) their ability to intercalate the DNA and to bind it within the minor groove in different orientations. DNA-ligand complexes are characterized by the length of the ligand binding site on the DNA lattice (so-called "multiple-contact" model). We show here that if two or more complexes with different lengths of the ligand binding sites could be produced by the same ligand, the dependence of the concentration of the complex with the shorter length of binding site on the total concentration of ligand should be S-shaped. Our theoretical model is confirmed by comparison of the calculated and experimental CD binding curves for bis-netropsin binding to poly(dA-dT) poly(dA-dT). Bis-netropsin forms two types of DNA complexes due to its ability to interact with the DNA as monomers and trimers. Experimental S-shaped bis-netropsin-DNA binding curve is shown to be in good correlation with those calculated on the basis of our theoretical model. The present work provides new insight into the analysis of ligand-DNA binding curves.     

Cooperation effects in binding of large ligands to DNA. II. Contact interactions between adsorbed ligands

Cooperative effects arising upon binding of biologically active ligands to DNA are considered. Equations are derived which enable one to describe the binding of two different ligands to DNA. We also consider the case when ligand can form two type of DNA complexes. The cooperative binding of the ligand in the vicinity of saturation level of binding can be described with a good accuracy by equation derived for the non-cooperative adsorption of the same ligand with some effective binding constant Keff. It is shown that cooperative effects arising upon binding of proteins and other ligands to DNA can be divided into two groups depending on the symmetry of interactions between the bound ligand molecules. In particular, if such interactions favor the formation of dimeric ligand species on the DNA, Keff approximately a1/2, where a is the ligand-ligand interaction constant. If cooperative interactions favor the formation of aggregates of unrestricted size, then Keff approximately aL+Y, where L is the size of the binding site for the ligand on DNA.     

Theoretical calculations of the helix–coil transition of DNA in the presence of large,cooperatively binding ligands

Theoretical calculations are conducted on the helix–coil transition of DNA, in the presence of large, cooperatively binding ligands modeled after the DNA-binding proteins of current biological interest. The ligands are allowed to bind both to helx and to coil, to cover up any number of bases or base pairs in the complex, and to interact cooperatively with their nearest neighbors. The DNA is treated in the infinite homogeneous Ising model approximation, and all calculations are done by Lifson's method of sequence-generating functions. DNA melting curves are calculated by computer in order to expolore the effects on the transition of ligand size, binding constant, free activity, and ligand–ligand cooperativity. The calculations indicate that (1) at the same intrinsic free energy change per base pair of the complexes, small ligands, for purely entropic reasons, are more effective than are large ligands in shifting the DNA melting temperature; (2) the response of the DNA melting temperature to increased ligand binding constant K and/or free ligand activity L is adequately represented at high values of KL (but not at low KL) by a simple independent site model; (3) if curves are calculated with the total amount of added ligand remaining constant and the free ligand activity allowed to vary throughout the transition, biphasic melting curves can be obtained in the complete absence of ligand–ligand cooperativity. In an Appendix, the denaturation of poly[d(A-T)] in the presence of the drug, netropsin, is used to verify some features of the theory and to illustrate how the theory can be used to obtain numerical estimates of the ligand binding parameters from the experimental melting curves.     

Study of the interaction of Co(III) polypyridyl complexes with DNA: an experimental and computational approach

Three new cobalt(III) polypyridyl complexes, [Co(L - L)₂IIP]³⁺ where IIP = 2-(2H-isoindol-1-yl)-2H-imidazo[4,5-f][1, 10]phenanthroline, L?=?1) phen (1,10-phenanthroline), 2) bpy (2,2’bipyridyl), 3) dmb (4, 4-dimethyl 2, 2’-bipyridine) have been synthesized, characterized (UV –VIS, IR, ¹HNMR and ¹³C NMR spectroscopy) and screened for their in vitro antibacterial activity against E.coli, Staphylococcus aureus and Bacillus subtilis. The binding of these complexes with calf-thymus DNA (CT-DNA) has been investigated by absorption and fluorescence spectroscopy, viscosity measurements. The experimental studies indicate that complexes bind to CT-DNA by means of intercalation, but with different binding affinities due to differences in the planarity of the ancillary ligand. The complexes promote photocleavage of plasmid DNA from super coiled form I to the open circular form II. The antibacterial activities suggest that the metal complexes are more active as compared to the prepared un-complexed IIP ligand.

In addition, a conformational search was carried out by Molecular Dynamics Simulations, and docking revealed that complexes intercalate between base pairs of DNA. The experimental and computational approaches reveal that the length of the intercalator and the nature of ancillary ligand are highly important factors for DNA binding.     

Curves of ligand binding. The use of hyperbolic functions for expressing titration curves

1. The dependences of the concentrations of the non-ligated, uni-ligated and bi-ligated forms of a molecule that binds two molecules of ligand are expressed as functions of the logarithm of free ligand concentration by means of hyperbolic functions. Expressions are also given for the saturation both of an individual site and of the molecule as a whole. This form of expression allows derivation of the following points. 2. The sharpness of bell-shaped curves of concentration of the uni-ligated form is analysed in terms of the heights of their points of inflexion; these can rise to 1/ radical2 of the curve. 3. A single group can exhibit a doubly sigmoid saturation curve if this group and another have comparable affinities for a ligand, and if ligand binding at one of them diminishes the affinity at the other. If the molecular pK values pK(1) and pK(2) for the first and second molecules of ligand are called pK*+/-logm, so that K*(2)=K(1)K(2) and m(2)=K(1)/K(2), then the doubly sigmoid curve can be represented by the sum of two independent one-site saturation curves, in general of unequal height, of pK values pK*+/-log(1/2)[m+ radical(m(2)-4)]. The error in such representation is small either if the mutual interaction between the groups (i.e. m) is large, or if the groups have very similar affinities for the ligand. 4. The sum of two one-site saturation curves, again of pK values of pK*+/-log(1/2)[m+ radical(m(2)-4)] but of equal heights, gives a precise value for the total saturation, provided that the binding of one molecule does not promote the binding of a second, i.e. providing that m>/=2. Hence determinations of saturation cannot distinguish interacting and possibly identical sites from independent and different ones.     

Modeling of DNA condensation and decondensation caused by ligand binding

A theoretical method for computer modeling of DNA condensation caused by ligand binding is developed. In the method, starting (s) and condensed (c) states are characterized by different free energies for ligand free DNA (F(s) and F(c) respectively), ligand binding constants (K(s) and K(c)) and stoichiometry dependent parameters (c(sm) and c(cm) - maximum relative concentration of bound ligands (per base pair) for starting and condensed state respectively). The method allows computation of the dependence of the degree of condensation (the fraction of condensed DNA molecules) on ligand concentration. Calculations demonstrate that condensation transition occurs under an increase in ligand concentration if F(s) < F(c) (i.e. S(sc) = exp [- (F(c) - F(s)) / (RT)], the equilibrium constant of the s-c transition, is low (S(sc) < 1)) and K(s) < K(c). It was also found that condensation is followed by decondensation at high ligand concentration if the condensed DNA state provides the number of sites for ligand binding less than the starting state (c(sm) > c(cm)). A similar condensation-decondensation effect was found in recent experimental studies. We propose its simple explanation.     

DNA Interaction and Photocleavage Properties of Ru (II) Complexes [Ru(bpy)2(pibi)]2+ and [Ru(phen)2(pibi)]2+

A new asymmetry ligand pibi (pibi = 2-(pyridine-2-yl)-1-H-imidazo[4,5-f]benzo[d]imidazolone) and its ruthenium complexes with [Ru(L)₂(pibi)]²⁺ (L = bpy (2, 2′-bipyridine), phen (1, 10-phenanthroline)), have been synthesized and characterized. The binding of two complexes with calf thymus DNA has been investigated by spectroscopic and viscosity measurement. The results indicate that both complexes can bind to CT-DNA through intercalative mode. Under irradiation at 365 nm, both complexes can partly promote the photocleavage of plasmid pBR322DNA. The low singlet oxygen generation abilities of the two complexes may be the factor for the low DNA photocleavage abilities.     

Copper(II) complexes of tridentate pyridylmethylethylenediamines: role of ligand steric hindrance on DNA binding and cleavage

Copper(II) complexes of three linear unsymmetrical tridentate ligands viz. N-methyl-N'-(pyrid-2-ylmethyl)ethylenediamine (L1), N,N-dimethyl-N'-(pyrid-2-ylmethyl)ethylenediamine (L2) and N,N-dimethyl-N'-((6-methyl)pyrid-2-ylmethyl)ethylenediamine (L3) have been isolated and characterized by elemental analysis, electronic absorption and EPR spectroscopy and cyclic and differential pulse voltammetry. Of these complexes [Cu(L2)Cl2] and [Cu(L3)Cl2] have been structurally characterized by X-ray crystallography. The [Cu(L2)Cl2] complex crystallizes in the monoclinic space group P2(1)/n with a=11.566(2) A, b=7.369(1) A, c=15.703(3) A, alpha=90 degrees , beta=109.68(8) degrees , gamma=90 degrees and Z=4 while [Cu(L3)Cl2] crystallizes in the triclinic space group P1 with a=9.191(2) A, b=12.359(3) A, c=14.880(3) A, alpha=79.61(13) degrees , beta=86.64(13) degrees , gamma=87.28(8) degrees and Z=2. The coordination geometries around copper (II) in these two complexes are best described as trigonal bipyramidal distorted square based pyramidal (TBDSBP). The distorted CuN3Cl basal plane in them is comprised of three nitrogen atoms of the meridionally coordinated ligand and a chloride ion and the axial position is occupied by the other chloride ion. The interaction of these complexes with Calf Thymus DNA (CT DNA) has been studied by using absorption, emission and circular dichroic spectral methods, thermal denaturation studies, viscometry and cyclic and differential pulse voltammetry. A strong blueshift in the ligand field band and a redshift in the ligand based bands of the copper(II) complexes on binding to DNA imply a covalent mode of DNA binding of the complexes, which involves coordination of most possibly guanine N7 nitrogen of DNA to form a CuN4 chromophore. This is supported by studying the interaction of the complexes with N-methylimidazole (N-meim), guanosine monophosphate (GMP), adenosine monophosphate (AMP) and cytidine (cytd) by ligand field and EPR spectral methods, which indicate the formation of a CuN4 chromophore only in the case of the more basic N-meim and GMP. The DNA melting curves obtained in the presence of copper(II) complexes reveal a monophasic and irreversible melting of the DNA strands and the high positive DeltaTm values (12-21 degrees C) also support the formation of strong Cu-N bonds by the complexes with DNA, leading to intra- and/or interstrand crosslinking of DNA. Competitive ethidium bromide (EthBr) binding studies show that the L2 and L3 complexes are less efficient than the L1 complex in quenching EthBr emission, which is consistent with their forming DNA crosslinking preventing the displacement of the DNA-bound EthBr. A very slight decrease in relative viscosity of DNA is observed on treating the L1 and L2 complexes with CT DNA; however, a relatively significant decrease is observed for the L3 complex suggesting that the length of the DNA fiber is shortened. DNA cleavage experiments show that all the complexes induce the cleavage of pBR322 plasmid DNA, the complex of L1 being more efficient than those of sterically hindered L2 and L3 ligands.     

"Bridge" structures between nucleic acid molecules fixed in the structure of a liquid crystal

The binding of daunomycin and copper ions to poly(I).poly(C) molecules fixed in a particle of a liquid-crystalline dispersion was studied. A thermodynamic model of adsorption was developed, which makes it possible to describe the formation of complexes of a particular kind, "bridges" that connect adjacent nucleic acid molecules fixed in a liquid crystal. The bridges represent chelate complexes, which incorporate the molecules of the antibiotic daunomycin and copper ions. Equations describing the dependence of the concentration of these bridges in solution on the concentration of their constituents were derived. The family of dependences of experimental amplitudes of bands in CD spectra typical of "bridge" structures on the concentration of copper ions represents a set of S-shaped curves, and, as the concentration of daunomycin in solution increases, the level of saturation of these curves increases. The analysis of experimental data with the use of this model suggests that the structures of this type compete with daunomycin molecules for the binding sites on poly(I).poly(C). By using this model, the energies of formation of bridge structures were calculated.     

Requirements for reliable determination of binding affinity constants by saturation analysis approach

Accurate calculation of the equilibrium association constant (K) and binding site concentration (N) related to a receptor (R)/ligand (L) interaction, via R saturation analysis, requires exact determination of the specifically bound L concentration (B(S)) and the unbound L concentration (U) at equilibrium. However, most binding determinations involve a procedure for separation of bound and unbound L. In such situations, it was previously shown that correct calculation of B(S) and U from binding data requires prior determination of alpha, i.e. the procedure parameter representing the proportion of equilibrium B(S) recovered after running the separation process, and of kn, i.e. the equilibrium nonspecific binding coefficient. For the simplest model of R/L interaction, the consequences of alpha neglect and/or kn neglect on determination of K and N, via R saturation analysis, are investigated. When alpha but not kn has been determined, B(S) can be accurately calculated, whereas U is overestimated by factor (kn + 1). Consequently the type (linear or hyperbolic) of theoretic curves obtained by usual representations (such as the Scatchard, the Lineweaver-Burk or the Michaelis-Menten plot) of the R/L binding is unchanged; these curves afford correct N and underestimation of K by factor (kn + 1). When alpha (alpha < 1) has not been determined B(S) and U are underestimated and overestimated, respectively. Then erroneous representations of the R/L binding result (e.g. instead of regular straight line segments, Scatchard plot and Lineweaver-Burk plot involve convex-upward and convex-downward hyperbola portions, respectively, suggestive of positive cooperativity of L binding), which leads to incorrect N and K. Errors in N and K would depend on (i) the binding (K, N and kn) and method (alpha) parameters and (ii) the expressions used to calculate approximate B(S) and U values. Simulations involving variable alpha, KN and kn values indicate that: (1) the magnitude of error in N determination (mainly involving moderate underestimation) directly depends on the alpha value; (2) the magnitude of K underestimation mainly depends on the KN value; it is moderate (usually < two-fold) with KN values < 1, but could become very high (e.g. > 100-fold), when KN > 10(2). In this case, the K underestimation is modulated by the alpha and kn values. Practical situations which afford high KN and thus might result in very marked underestimation of K are discussed. A single R dilution method is proposed to assess the validity of K determinations using the R saturation analysis approach.     

Chromatin methylation activity of Dnmt3a and Dnmt3a/3L is guided by interaction of the ADD domain with the histone H3 tail

Using peptide arrays and binding to native histone proteins, we show that the ADD domain of Dnmt3a specifically interacts with the H3 histone 1–19 tail. Binding is disrupted by di- and trimethylation of K4, phosphorylation of T3, S10 or T11 and acetylation of K4. We did not observe binding to the H4 1–19 tail. The ADD domain of Dnmt3b shows the same binding specificity, suggesting that the distinct biological functions of both enzymes are not related to their ADD domains. To establish a functional role of the ADD domain binding to unmodified H3 tails, we analyzed the DNA methylation of in vitro reconstituted chromatin with Dnmt3a2, the Dnmt3a2/Dnmt3L complex, and the catalytic domain of Dnmt3a. All Dnmt3a complexes preferentially methylated linker DNA regions. Chromatin substrates with unmodified H3 tail or with H3K9me3 modification were methylated more efficiently by full-length Dnmt3a and full-length Dnmt3a/3L complexes than chromatin trimethylated at H3K4. In contrast, the catalytic domain of Dnmt3a was not affected by the H3K4me3 modification. These results demonstrate that the binding of the ADD domain to H3 tails unmethylated at K4 leads to the preferential methylation of DNA bound to chromatin with this modification state. Our in vitro results recapitulate DNA methylation patterns observed in genome-wide DNA methylation studies.     

Molecular dynamics simulations and binding free energy analysis of DNA minor groove complexes of curcumin

Curcumin is a natural phytochemical that exhibits a wide range of pharmacological properties, including antitumor and anticancer activities. The similarity in the shape of curcumin to DNA minor groove binding drugs is the motivation for exploring its binding affinity in the minor grooves of DNA sequences. Interactions of curcumin with DNA have not been extensively examined, while its pharmacological activities have been studied and documented in depth. Curcumin was docked with two DNA duplexes, d(GTATATAC)₂ and d(CGCGATATCGCG)₂, and molecular dynamics simulations of the complexes were performed in explicit solvent to determine the stability of the binding. In all systems, the curcumin is positioned in the minor groove in the A·T region, and was stably bound throughout the simulation, causing only minor modifications to the structural parameters of DNA. Water molecules were found to contribute to the stability of the binding of the ligand. Free energy analyses of the complexes were performed with MM-PBSA, and the binding affinities that were calculated are comparable to the values reported for other similar nucleic acid–ligand systems, indicating that curcumin is a suitable natural molecule for the development of minor groove binding drugs.     

Structure–activity relationship study of copper(II) complexes with 2-oxo-1,2-dihydroquinoline-3-carbaldehyde (4′-methylbenzoyl) hydrazone: synthesis, structures, DNA and protein interaction studies, antioxidative and cytotoxic activity

Novel 2-oxo-1,2-dihydroquinoline-3-carbaldehyde (4′-methylbenzoyl) hydrazone (H₂L) (1) and its two copper(II) complexes have been synthesized. Single-crystal X-ray diffraction studies revealed that the structure of the new copper(II) chloride complex, [Cu(H₂L)Cl₂]·2H₂O (2), is square pyramidal and that of the copper(II) nitrate complex, [Cu(HL)NO₃]·DMF (3), is square planar. In 2, the copper atom is coordinated by the ligand with ONO donor atoms, one chloride ion in the apical position, and the other chloride in the basal plane. In 3, the ligand coordinates as a uninegative tridentate ONO⁻ species and with one nitrate ion in the basal plane. DNA binding experiments indicated that the ligand and copper(II) complexes can interact with DNA through intercalation. Bovine serum albumin binding studies revealed that the compounds strongly quench the intrinsic fluorescence of bovine serum albumin through a static quenching process. Antioxidative activity tests showed that 1 and its copper(II) complexes have significant radical scavenging activity against free radicals. Cytotoxic activities of the ligand and copper(II) complexes showed that the two copper(II) complexes exhibited more effective cytotoxic activity against HeLa and HEp-2 cells than the corresponding ligand. The entire biological activity results showed that the activity order was 1 < 2 < 3.     

Synthesis, crystal structure and DNA-binding studies of the Ln(III) complex with 6-hydroxychromone-3-carbaldehyde benzoyl hydrazone

A novel 6-hydroxy chromone-3-carbaldehyde benzoyl hydrazone ligand (L) and its Ln(III) complexes, [Ln=La(1) and Sm(2)], have been prepared and characterized. The crystal and molecular structures of complexes 1 and 2 were determined by single-crystal X-ray diffraction. Antioxidative activity tests in vitro showed that L and its complexes have significant antioxidative activity against hydroxyl free radicals from the Fenton reaction and also oxygen free radicals, and that the effect of the La(III) complex 1 is stronger than that of mannitol and the other compounds. The compounds were tested against tumor cell lines including HL-60 and A-549. The data shows that the suppression rate of complexes 1 and 2 against the tested tumor cells are superior to the free ligand (L). The interactions of complexes 1 and 2, and L, with calf thymus DNA were investigated by UV-visible (UV-vis), fluorescence, denaturation experiments and viscosity measurements. Experimental results indicated that complexes 1 and 2, and L can bind to DNA via the intercalation mode, and that the binding affinity of complex 1 is higher than that of complex 2 and of free ligand (L). The intrinsic binding constants of complexes 1 and 2, and L were (7.62+/-0.56)x10(6), (3.70+/-0.47)x10(6) and (2.41+/-0.46)x10(6)M(-1), respectively.     

A spectroscopic investigation of the self-association and DNA binding properties of a series of ternary ruthenium(II) complexes

Six ruthenium(II) complexes of the general form cis-alpha-[Ru(N4-tetradentate)(N2-bidentate)]Cl2 have been synthesized from the two related tetradentate ligands 1,6-di(2'-pyridyl)-2,5-dimethyl-2,5-diazahexane (picenMe2) and 1,6-di(2'-pyridyl)-2,5-dibenzyl-2,5-diazahexane (picenBz2) and the bidentate ligands 2,2'-bipyridine (bipy), 1,10-phenanthroline (phen) and dipyrido[3,2-f:2'3'-h]quinoxaline (dpq). Synthetic intermediate species of the general form cis-alpha-[Ru(II)(N4-tetradentate)(DMSO)Cl][PF6] were isolated. The N4-tetradentate ligand picenMe2 formed only the cis-alpha stereoisomer, while picenBz2 formed both the cis-alpha and cis-beta stereoisomers. These latter stereoisomers were resolved by fractional crystallisation. Dimer self-association constants, K(D), were estimated from the concentration dependence of the 1H NMR shifts for some of these complexes in aqueous solutions at 25 degrees C. The values of K(D) ranged from 0.6 to 7.9 M(-1) and a relationship was observed between the aromatic surface area of the bidentate component and the degree to which self-association occurred, whereby a greater level of self-association correlates with a larger surface area for the bidentate ligand. Some of these complexes demonstrate an ability to bind to DNA that is consistent with intercalation of the bidentate molecular component between the base pairs of the DNA molecule. Using calf-thymus DNA, the equilibrium binding constants, K(B), were determined for some of the complexes using intrinsic methods and these ranged from 3.32 to 5.11 M(-1), the intercalating abilities of the different bidentate ligands being in the order dp q > phen > bipy. This relationship between aromatic surface area of the bidentate ligand and the degree of DNA binding activity is the same as that observed in the self-association study.     

Synthesis, DNA binding, and oxidative cleavage studies of Fe(II) and Co(III) complexes containing bioactive ligands

The two complexes containing bioactive ligands of the type and [Fe(L)] (PF(6))(2) (1) (where L = [1-{[2-{[2-hydroxynaphthalen-1-yl)methylidine]amino}phenyl)imino] methyl}naphthalene-2-ol]) and [Co(L(1)L(2))] (PF(6))(3) (2) (where L(1)L(2) = mixed ligand of 2-seleno-4-methylquinoline and 1,10-phenanthroline in the ratio 1:2, respectively) were synthesized and structurally characterized. The DNA binding property of the complexes with calf thymus DNA has been investigated using absorption spectra, viscosity measurements, and thermal denaturation experiments. Intrinsic binding constant K(b) has been estimated at room temperature. The absorption spectral studies indicate that the complexes intercalate between the base pairs of the CT-DNA tightly with intrinsic DNA binding constant of 2.8 × 10(5) M(-1) for (1) and 4.8 × 10(5) M(-1) for (2) in 5 mM Tris-HCl/50 mM NaCl buffer at pH 7.2, respectively. The oxidative cleavage activity of (1) and (2) were studied by using gel electrophoresis and the results show that complexes have potent nuclease activity.     

Binding of oxovanadium ions to the major and minor grooves of DNA duplex: stability and structural models.

Vanadate induces DNA strand breaks in cultured human fibroblasts at doses that are relative to the occupational exposure. Oxovanadium compounds also exert preventive effects against chemical carcinogenesis in animals and form complexes with DNA in vivo. This study was designed to examine the interaction of calf-thymus DNA with VO2+ and VO3 ions in aqueous solution at physiological pH, with a constant DNA concentration of 12.5 mmol/L and vanadium-DNA (phosphate) molar ratios (r) of 1:160 to 1:2. Capillary electrophoresis and Fourier transform infrared difference spectroscopy were used to determine the cation binding site, the binding constant, the helix stability, and DNA conformation in the oxovanadium-DNA complexes. Structural analysis showed that VO2+ binds DNA through guanine and adenine N-7 atoms and the backbone PO2 group with apparent binding constants of KG = 8.8 x 10(5) (mol/L)-1 and KA = 3.4 x 10(5) (mol/L)-1. The VO3 shows weaker binding through thymine, adenine, and guanine bases, with K = 1.9 x 10(4) (mol/L)-1 and no interaction with the backbone phosphate group. A partial B-to-A DNA transition occurred upon VO-DNA complexation, while DNA remains in the B-family structure in the VO3 complexes.     

DNA binding affinity and antioxidative activity of copper(II) and zinc(II) complexes with a novel hesperetin Schiff base ligand

A hesperetin Schiff base ligand (H₄L) and its complexes, [H₃CuL·OAc]·H₂O and [H₃ZnL·OAc]·2H₂O, have been synthesized and characterized on the basis of elemental analysis, molar conductivity, ¹H NMR, mass spectra, UV-Vis spectra and IR spectra. The binding of these two complexes and the ligand to DNA has been investigated by ultraviolet absorption spectroscopy, fluorescence spectroscopy and viscosity measurements. The experiments indicate that all the compounds can bind to DNA through an intercalative mode and the complexes intercalate into DNA more deeply than that of the ligand. In addition, the antioxidative activity was also determined. The 50% inhibition obtained for the ligand and its complexes demonstrates that, compared to the ligand, the complexes exhibit higher antioxidative activity in the suppression of and HO.