On the triplet states of polynucleotide--acridine complexes. I. Triplet energy delocalization in the 9-aminoacridine-DNA complex

Phosphorescence and fluorescence from the dye in complexes of DNA with 9-amino-acridine and acridine orange in a glycerol-H₂O glass have been measured at 77°K. The dependence of the p/fratio for 9-aminoacridine on the exciting wavelength demonstrates triplet–triplet energy transfer from DNA to dye. The result provides evidence for π electron overlap between the dye and the bases of native DNA. The observation that the magnitude of the enhancement in ultraviolet-excited dye phosphorescence increases with the base to dye ratio indicates triplet delocalization in the polymer. Preliminary flash experiments provide evidence that this delocalization is not limited by slow diffusion of the triplet exciton. The inability to detect transfer on denaturation of the DNA illustrates the sensitivity of triplet–triplet energy transfer to the conformation of the macromolecular complex.     

Über die Vitalfluorochromierung des Kernchromatins und der Chromosomen von HeLa-Zellen mit AMHA und die Bindung des Acridinfarbstoffs an DNA

Summary The fluorochrome AMHA (3-amino-6-methoxy-9-(2-hydroxyethylamino)acridine) stains the nuclear chromatin and the chromosomes of living HeLa cells. At relatively low dye concentrations C _F10^–4 M and short incubation periods t _I2 h cell growth is not affected by the drug. But at higher C _F and longer t _I the population doubling time of the cell cultures rapidly increases, and finally the cells die.In vital staining experiments the dye AMHA preferentially binds to the DNA of the nuclei and to the chromosomes of the cells, respectively. The dye binding to DNA has been proved by the absorption and emission microspectra of the stained cells, and by the comparison with authentic spectra of AMHA bound to DNA in aqueous solutions. Within the limits of experimental errors both types of spectra are identical. The spectra of DNA-bound AMHA show a characteristic gap of ca. 3500 cm^–1 between the 0-0-transitions of the long wave length ¹ L _a absorption and the fluorescence. AMHA molecules dissolved in the polar solvent water have a gap of even 4100 cm^–1. This energy gap shows that the electron distribution of AMHA is strongly changed by light absorption and emission.Finally, using absorption spectroscopy, we investigated the binding of AMHA to DNA in aqueous solutions over a wide range of concentrations of the dye, of nuceleic acid (calf thymus), and of the competitor NaCl respectively. The Scatchard binding isotherms were determined. With the method of competitive salt effect three different bonds of AMHA to DNA can be distinguished even at low dye concentrations: The intercalation 1 of the fluorochrome F, binding constant K _F1=1,1·10⁵ M ^–1, binding parameter n ₁=0,15; the pre-intercalative or external binding 2, K _F2=6,9·10⁵ M ^–1, n ₂=0,21; the external binding 3, K _F3=2,8·10⁵ M ^–1, n ₃=0,55. Externally bound dye molecules 2 and 3 occupy two phosphodiester residues of the DNA. A detailed discussion of the data and the competitive salt effect shows that in living cells only intercalated and small amounts of pre-intercalatively bound molecules 1 and 2 exist. The binding constant K _F1=1,1·10⁵ M ^–1 of AMHA is unusual high in comparison with the constants of intercalation of other dyes, K _F1=(1–4)·10⁴ M ^–1. Therefore, the amount of intercalated AMHA is also relatively high, and it is possible to visualize the DNA-bound fluorochrome in the nuclei and chromosomes of the living cells under the fluorescence microscope.     

Ultraviolet spectra of the complexes of acridine orange with deoxyribonucleic acid and polyphosphates

Summary Two kinds of changes were found in ultraviolet spectrum of acridine orange bound to polyphosphate and native or denatured DNA: (a) changes similar to those caused by aggregation in the solutions of pure acridine orange (i.e. blue shifts of the bands at 37300 cm^–1 and 43670 cm^–1, a decrease of absorbance of the band at 34600 cm^–1 and an increase of absorbance of the band at 43670 cm^–1), which were observed at those ratiosP/D, when the dye formed aggregates on the surface of the polyanion; (b) a decrease of absorbance in the whole near ultraviolet region, which had high value even when isolated dye molecules were bound to the polyanion. While the first kind of changes is due to mutual interactions between the aggregated acridine orange molecules, the second kind can be explained as due to interaction of the dye molecules with adjacent chromophores of the polyanion and/or solvent. The maximum value of the hypochromic effect in the near ultraviolet maximum was higher for complexes of denatured DNA than for complexes of native DNA.     

Fluorescence decay studies of the DNA-3,6-diaminoacridine complexes

The interaction of several 3,6-diaminoacridines with DNAs of various base composition has been studied by steady-state and transient fluorescence measurements. The acridine dyes employed are of the following two classes: class I - proflavine, acriflavine and 10-benzyl proflavine; class II - acridine yellow, 10-methyl acridine yellow and benzoflavine. It is found that the fluorescence decay kinetics follows a single-exponential decay law for free dye and the poly[d(A-T)]-dye complex, while that of the dye bound to DNA obeys a two-exponential decay law. The long lifetime (tau 1) for each complex is almost the same as the lifetime for the poly[d(A-T)]-dye complex, and the amplitude alpha 1 decreases with increasing GC content of DNA. The fluorescence quantum yields (phi F) of dye upon binding to DNA decrease with increasing GC content; the phi F values for class I are nearly zero when bound to poly(dG) X poly(dC), but those for class II are not zero. This is in harmony with the finding that GMP almost completely quenches the fluorescence for class I, whereas a weak fluorescence arises from the GMP-dye complex for class II. The fluorescence spectra of the DNA-dye complexes gradually shift toward longer wavelengths with increasing GC content. In this connection, the fluorescence decay parameters show a dependence on the emission wavelength; alpha 1 decreases with an increase in the emission wavelength. In view of these results, it is proposed that the decay behavior of the DNA-dye complexes has its origin in the heterogeneity of the emitting sites; the long lifetime tau 1 results from the dye bound to AT-AT sites, while the short lifetime tau 2 is attributable to the dye bound in the vicinity of GC pairs. Since GC pairs almost completely quench the fluorescence for class I, partly intercalated or externally bound dye molecules may play an important role in the component tau 2.     

Kinetics of proflavin binding to bacteriophages T2L and T4D

We have measured the kinetics of proflavin binding to T-even bacteriophages—the 700 S and 1000 S forms of T2L, T4D, and T4D os41—by difference spectroscopy at 430 nm. Measurements were carried out from 22° to 37°C. Binding is very slow to encapsulated DNA compared to free DNA, requiring hours to reach equilibrium. The kinetic data are compatible with the two-step mechanism where P is proflavin, N is nucleotide, and PN₁ and PN₂ are complexes. Computer integration of the rate equations allows evaluation of the rate constants; previous equilibrium measurements gave thermodynamic parameters. For all phage studied, the bimolecular step is endothermic with high positive entropy; the second, unimolecular step is highly exothermic with small negative entropy change. Both forms of T2L bind proflavin with essentially the same rate, as do T4D and the osmotic shock resistant mutant T4D os41. This suggests that the encapsulated DNA is equally accessible to proflavin in both forms of each phage. However, T4D binds dye appreciably faster than T2L, indicating that capsid permeability or DNA environment (glucosylation or packing) is different in the two species.     

Interaction of the antimalarial drug fluoroquine with DNA,tRNA, and poly(A): 19F-NMR chemical-shift and relaxation,optical absorption,and fluorescence studies

The interaction of the fluorinated antimalarial drug fluoroquine [7-fluoro-4-(diethyl-amino-1-methylbutylamino)quinoline] with DNA, tRNA, and poly(A) has been investigated by optical absorption, fluorescence, and ¹⁹F-nmr chemical-shift and relaxation methods. Optical absorption and fluorescence experiments indicate that fluoroquine binds to nucleic acids in a similar manner to that of its well-known analog chloroquine. At low drug-to-base pair ratios, binding of both drugs appears to be random. Fluoroquine and chloroquine also elevate the melting temperature (T_m) of DNA to a comparable extent. Binding of fluoroquine to DNA, tRNA, or poly(A) results in a downfield shift of about 1.5 ppm for the ¹⁹F-nmr resonance. The chemical shift of free fluoroquine depends on the isotopic composition of the solvent (D₂O vs H₂O). The solvent isotope shift is virtually eliminated by fluoroquine binding to any one of the nucleic acids. ¹⁹F-nmr relaxation experiments were carried out to measure the spin-lattice relaxation time (T₁), ¹⁹F{¹H} nuclear Overhauser effect (NOE), off-resonance intensity ratio (R), off-resonance rotating-frame spin-lattice relaxation time (T), and linewidth for fluoroquine in the nucleic acid complexes. By accounting for intramolecular proton-fluorine dipolar and chemical-shift anisotropy contributions to the fluorine relaxation, all of the relaxation parameters for the fluoroquine–DNA complex can be well described by a motional model incorporating long-range DNA bending on the order of a microsecond and an internal motion of the drug on the order of a nanosecond. Selective NOE experiments indicate that the fluorine in the drug is near the ribose protons in the RNA complexes, but not in the DNA complex. Details of the binding evidently differ for the two types of nucleic acids. This study provides the foundation for an investigation of fluoroquine in intact cells.     

Thermodynamics of mucopolysaccharide–dye binding. II. Binding constant and cooperativity parameters of acridine orange–dermatan sulfate system

In the acridine orange–dermatan sulfate system, free and bound dye can be distinguished from each other spectroscopically. This permits the use of fluorometric methods to study the binding of acridine orange to the acid mucopolysaccharide dermatan sulfate. Experiments were conducted at 24°C in 10^?3 M citrate/phosphate buffer at pH = 7.0. The binding of the dye is highly cooperative, as evidenced by considerable interaction between adjacent bound dye molecules. Analysis of the data indicates that dermatan sulfate binds 2.3 ± 0.3 mol of acridine orange per dermatan sulfate uronic acid residue with a cooperative binding constant, K_q ranging from 4.9 to 6.0 × 10⁵ M^?1 which corresponds to a free energy of 7.74 ? ΔG° ? 7.86. The cooperativity parameter q apparently increases with increasing polymer-to-dye ratio.     

Rate constants and activation parameters for the mobility of bulk and DNA-associated glycol-water solvents

The decrease in mobility of viscous glycol–water solvents when associated with native DNA is quantified from a study of the loss of the exciting-wavelength dependence of the phosphorescence spectrum of free and bound proflavin with increasing temperature. The data are interpreted in terms of a distribution of rate constants with an Arrhenius temperature dependence. Over the temperature range of the experiments a relative decrease of ～ 10⁴ in the average rate constant is observed for reorientation of the solvent when associated with DNA. The basis for this large reduction is found to derive from a large decrease in the pre-exponential factors (i.e., activation entropy) associated with the reorientation rate constants. The changes in the distribution of rate constants and the activation parameters for solvent mobility induced by DNA do not resemble the changes observed for any one of a number of small ion or molecule perturbations. The results suggest the presence of disorganized, relatively immobile solvent in association with DNA.     

Effect of organic solvents on the properties of the complexes of DNA with proflavine and similar compounds

In order to obtain information on the binding forces involved in the formation of the complex proflavine–DNA by the stronger process I, the stability of the complexes was investigated in the presence of various organic solvents, methanol, ethanol, n-propanol, isopropanol, formamide, dimethyl sulfoxide, p-dioxane, glycerol, and ethylene glycol. Quantitative data on binding in terms of K/n and r were obtained by means of absorption and fluorescence spectra, as well as by a thermal denaturation technique. All organic solvents used decrease the binding ability of the dye. The effectiveness of the solvents increases with their hydrocarbon content, but can hardly be related to their dielectric constant. The complex formation is effectively suppressed by organic solvent concentrations, in which DNA still preserves its double-helical conformation. These results demonstrate the importance of hydrophobic forces in the formation of the complex proflavine–DNA in aqueous solution. The similarity in spectroscopic properties of proflavine bound to DNA by process I and the same dye dissolved in an organic solvent make it possible to interpret the observed red shift of the long-wavelength absorption peak as being due to the interaction of the dye molecules with the less polar environment. The same behavior was found for other dyes capable of intercalation like purified trypaflavine, phenosafranine and ethidium bromide. However, intercalation is not a necessary condition, as it was shown in the case of pinacyanol, which binds only at the surface of DNA.     

Induced circular dichroism of acridine orange bound to double-stranded RNA and transfer RNA

The induced circular dichroism (CD) in the visible region of acridine orange bound to the double-stranded RNA from cytoplasmic polyhedrosis virus and to yeast tRNA has been measured as a function of RNA phosphate-to-dye ratio (P/D), under the conditions of 0.01 M Na⁺ at pH 7.0. The shape of the CD spectrum of acridine orange bound to the double-stranded RNA was quite different from the spectrum of the dye bound to DNA. The CD spectral features of acridine orange bound to the double-stranded regions in tRNA closely resembled those of the double-stranded RNA-dye complex, suggesting that the dyes bind similarly to the two RNA's. It was further found that the CD spectrum of the tRNA-dye complex at sufficiently high P/D ratios, which is assignable to monomeric, intercalated dye to the base-paired parts in tRNA, is also distinct from the corresponding spectrum of the DNA-dye complex.     

Electron donor properties of the antitumour drug amsacrine as studied by fluorescence quenching of DNA-bound ethidium

The effect of the antitumour acridine derivative amsacrine [4'-(9-acridinylamino)methanesulphon-m-anisidide] on the fluorescence lifetime of DNA-bound ethidium has been investigated using a synchronously pumped cavity dumped dye laser producing picosecond pulses for sample excitation and a time-correlated single photon counting detection system. As the proportion of DNA-bound amsacrine on the synthetic DNA polymer poly[deoxyadenylic-thymidylic acid] is increased, the fluorescence decay curve of ethidium can be accurately resolved into two exponential components. The short lifetime component, whose proportion increases with increasing proportions of DNA-bound amsacrine, has a lifetime of between 3 and 4 ns, significantly longer than that of ethidium in aqueous solution (1.63 ns). The magnitude of the long lifetime component decreases from 25.4 to 14 ns with increasing proportions of bound amsacrine. It is concluded that a new fluorescence state of ethidium (lifetime 3-4 ns) is present, probably resulting from reversible electron transfer between ethidium and amsacrine. The ability of various 9-anilinoacridine derivatives to quench the fluorescence of DNA-bound ethidium appears to be related to the electron donor properties of the substituents on the anilino ring, as well as to experimental antitumour activity. The electron donor properties of DNA-bound amsacrine may therefore be relevant to its antitumour action.     

Studies on poly(L-lysine50, L-tyrosine50)-DNA interaction

Interaction between poly(Lys⁵⁰, Tyr⁵⁰) and DNA has been studied by absorption, circular dichroism (CD), and fluorescence spectroscopy and thermal denaturation in 0.001M Tris, pH 6.8. The binding of this copolypeptide to DNA results in an absorbance enhancement and fluorescence quenching on tyrosine. There is also an increase in the tyrosine CD at 230 nm. The CD of DNA above 250 nm is slightly shifted to the longer wavelength which is qualitatively similar to, but quantitatively much smaller than, that induced by polylysine binding. At physiological pH the poly(Lys⁵⁰, Tyr⁵⁰)–DNA complex is soluble until there is one lysine and one tyrosine per nucleotide in the complex. The same ratio of amino acid residues to nucleotide has also been observed in copolypeptide-bound regions of the complex. The addition of more poly(Lys⁵⁰, Tyr⁵⁰) to DNA yields a constant melting temperature, T_m′, for bound base pairs at 90°C which is close to that of polylysine-bound DNA under the same condition. The melting temperature, T_m, of free base pairs at about 60°C on the other hand, is increased by 10°C as more copolypeptide is bound to DNA. As the temperature is raised, both absorption and CD spectra of the complexes with high coverage are changed, suggesting structural alteration, perhaps deprotonation, on bound tyrosine. The results in this report also suggest that intercalation of tyrosine in DNA is unlikely to be the mode of binding.     

The Binding of fd Gene 5 Protein to Polydeoxynucleotides: Evidence from CD Measurements for Two Binding Modes

Abstract

Circular dichroism measurements were used to study the binding of fd gene 5 protein to fd DNA, to six polydeoxynucleotides (poly(d(A)], poly[d(T)], poly[d(I)], poly[d(C)], poly[d(A-T)], and the random copolymer poly[d(A,T)]), and to three oligodeoxynucleotides (d(pA)₂₀, d(pA)₇, and d(pT)₇). Titrations of these DNAs with fd gene 5 protein were generally done in a low ionic strength buffer (5 mM Tris-HCl, pH 7.0 or 7.8) to insure tight binding, needed to obtain stoichiometric endpoints. By monitoring the CD of the nucleic acids above 250 nm, where the protein has no significant intrinsic optical activity, we found that there were two modes of binding, with the number of nucleotides covered by a gene 5 protein monomer (n) being close to either 4 or 3. These stoichiometrics depended upon which polymer was titrated as well as upon the protein concentration. Single endpoints at nucleotide/protein molar ratios close to 3 were found during titrations of poly[d(T)] and fd DNA (giving n = 3.1 and 2.8 ± 0.2, respectively), while CD changes with two apparent endpoints at nucleotide/protein molar ratios close to 4 and approximately 3 were found during titrations of poly[d(A)], poly[d(I)], poly[d(A-T)], and poly[d(A,T)) (with the first endpoints giving n = 4.1, 4.0, 4.0, and 4.1 ± 0.3, respectively). Calculations showed that the CD changes we observed during these latter titrations were consistent with a switch between two non- interacting binding modes of n = 4 and n = 3. We found no evidence for an n = 5 binding mode. One implication of our results is that the Brayer and McPherson model for the helical gene 5 protein-DNA complex, which has 5 nucleotides bound per protein monomer (G. Brayer and A. McPherson, J. Biomol Struct, and Dyn. 2, 495-510, 1984), cannot be correct for the detailed solution structure of the complex.

We interpreted the CD changes above 250 nm upon binding of the gene 5 protein to single-stranded DNAs to be the result of a slight unstacking of the bases, along with a significant alteration of the CD contributions of the individual nucleotides in the case of A- and/or T-containing DNAs, Interestingly, CD contributions attributed to nearest-neighbor interactions in free poly[d(A-T)], poly[d(A,T)], poly[d(A)], and poly[d(T)] were partially maintained in the CD spectra of the protein-saturated polymers, so that neighboring nucleotides, when bound to the protein at 20°C, appeared to interact with one another in much the same manner as in the free polymers at 50°C. Finally, we found that the protein tyrosyl CD band at 228.5 nm decreased 39-42% when the protein bound to poly[d(A)] or poly[d(T)], but this band decreased no more than 9% when the gene 5 protein bound to short A- or T-containing oligomers. Thus, at least one tyrosyl residue has a significantly altered optical activity only when the DNA substrate is long enough either to cause a transition to a different protein conformation or to allow additional protein-protein contacts between adjacent helical turns of the DNA-protein complex.     

Mechanism of acridine uptake by submitochondrial particles.

Acridines were compared regarding their ability to be taken up by submitochondrial particles under energized conditions. pH dependence of uptake was explored, and it was found that acridines fell into three classes independently of their pK_a value: acridines which are not taken up, acridines taken up at all pH values, and acridines taken up only at alkaline pH. Partition measurements between H₂O and chloroform phase showed a similar pattern, and affinity for the organic phase seemed to parallel uptake. Acridines which are taken up by submitochondrial particles at acidic pH under energized conditions despite a high pK_a value could also be extracted into chloroform at acidic pH, thus implying that the dye's uncharged form has a high affinity for the organic phase. By supplementing the aqueous medium with lipophilic anions, the dye may also be extracted in its charged form. The data support a mechanism for acridine uptake in which diffusion of the uncharged form across the membranes is an obligatory step. Some previously reported inhibitory anion effects on uptake may be explained by ion pair formation, which allows release of the accumulated charged form.     

Structure and stability of complexes formed by nucleic acids. I. Binding of acridine to DNA

Nuclear magnetic resonance spectra of acridine have been measured in aqueous methanol solutions over a wide concentration range in the presence and absence of dissolved DNA. In solutions containing DNA the acridine spectra show a marked line broadening and intensity decrease at temperatures lower than 50°C. These line-shape changes can be associated with two types of binding interactions: (1) a tight, irrotational binding of the acridine at low acridine:phosphate ratios and (2) a weaker, rotationally less restrictive binding at high acridine concentrations. At temperatures above 50°C. a marked line narrowing is noted for the acridine spectrum and is attributed to an increase in mobility of the bound acridine as the DNA complex undergoes a helix–coil transition. A loose association of acridine molecules with the purine and pyrimidine bases in heat-denatured DNA is indicated by chemical shift changes in the acridine spectrum. The NMR measurements also show that the presence of acridine in denatured DNA solutions greatly reduces renaturation of the 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.     

Microcalorimetric Investigation of DNA,poly(dA)poly(dT) and poly[d(A-C)]poly[d(G-T)] Melting in the Presence of Water Soluble (Meso tetra (4 N oxyethylpyridyl) Porphyrin) and its Zn Complex

Abstract

Thermodynamic parameters of melting process (δH_m, T_m, δT_m) of calf thymus DNA, poly(dA)poly(dT) and poly(d(A-C))·poly(d(G-T)) were determined in the presence of various concentrations of TOEPyP(4) and its Zn complex. The investigated porphyrins caused serious stabilization of calf thymus DNA and poly poly(dA)poly(dT), but not poly(d(A-C))poly(d(G-T)). It was shown that TOEpyp(4) revealed GC specificity, it increased T_m of satellite fraction by 24°C, but ZnTOEpyp(4), on the contrary, predominately bound with AT-rich sites and increased DNA main stage T_m by 18°C, and T_m of poly(dA)poly(dT) increased by 40 °C, in comparison with the same polymers without porphyrin. ZnTOEpyp(4) binds with DNA and poly(dA)poly(dT) in two modes—strong and weak ones. In the range of r from 0.005 to 0.08 both modes were fulfilled, and in the range of r from 0.165 to 0.25 only one mode—strong binding—took place. The weak binding is characterized with shifting of T_m by some grades, and for the strong binding T_m shifts by ～ 30–40°C. Invariability of ΔH_m of DNA and poly(dA)poly(dT), and sharp increase of T_m in the range of r from 0.08 to 0.25 for thymus DNA and 0.01–0.2 for poly(dA)poly(dT) we interpret as entropic character of these complexes melting. It was suggested that this entropic character of melting is connected with forcing out of H₂O molecules from AT sites by ZnTOEpyp(4) and with formation of outside stacking at the sites of binding. Four-fold decrease of calf thymus DNA melting range width ΔT_m caused by increase of added ZnTO- Epyp(4) concentration is explained by rapprochement of AT and GC pairs thermal stability, and it is in agreement with a well-known dependence, according to which ΔT～T_GC-T_AT for DNA obtained from higher organisms (L. V. Berestetskaya, M. D. Frank-Kamenetskii, and Yu. S. Lazurkin. Biopolymers 13, 193–205 (1974)). Poly (d(A-C))poly(d(G-T)) in the presence of ZnTOEpyp(4) gives only one mode of weak binding. The conclusion is that binding of ZnTOEpyp(4) with DNA depends on its nucleotide sequence.     

Modulation of DNA intercalation by resveratrol and genistein

Time correlated Single Photon Counting study (TCSPC) was performed for the first time to evaluate the effect of resveratrol (RES) and genistein (GEN) at 10–100 μM and 10–150 μM respectively, in modulating the DNA conformation and the variation induced due to intercalation by the dyes, ethidium bromide (EtBr) and acridine orange (AO). It is demonstrated using UV-absorption and fluorescence spectroscopy that RES and GEN, at 50 μM and 100 μM respectively can bind to DNA resulting in significant de-intercalation of the dyes, preventing their further intercalation within DNA. Hyperchromicity with red/blue shifts in DNA when bound to dyes was reduced upon addition of RES and GEN. DNA-dependent fluorescence of EtBr and AO was quenched in the presence of RES by 87.97% and 79.13% respectively, while similar quenching effect was observed for these when interacted with GEN (85.52% and 83.85%). It is found from TCSPC analysis that the higher lifetime component or constituent of intercalated dyes (τ₂, A ₂) decreased with the subsequent increase in smaller component or constituent of free dye (τ₁, A ₁) after the interaction of drugs with the intercalated DNA. Thus these findings signify that RES and GEN can play an important role in modulating DNA intercalation, leading to the reduction in DNA-directed toxicity.