Further fluorospectrophotometric studies on the binding of acridine orange with DNA. Effects of thermal denaturation of DNA and additions of spermine, kanamycin, dihydrostreptomycin, methylene blue and chlorpromazine

Fluorospectrophotometric studies on the binding of acridine orange (AO) with calf thymus DNA showed that the thermal denaturation of DNA reduced markedly the fluorescence of Complex II and the extent of this decrease depended on the temperature to which the DNA solutions were heated. The denaturation was carried out in the absence and presence of AO (methods A and B, respectively), and then fluorescence measurements of solutions were carried out at 23 °C. The fluorescence intensity-heating temperature curves obtained by methods A and B were similar in shape to the usual melting curves of DNA and AO-DNA solutions, respectively. The higher midpoint value obtained with method B indicates the stabilizing activity of AO against denaturation. These findings support an intercalation model for Complex II and an external self-association binding model for Complex I.A high concentration of ethylene diamine (EDA) restored the fluorescence of denatured Complex II to about 80% of the intensity value of native Complex II. The effects of spermine, kanamycin and dihydrostreptomycin were much stronger than that of EDA.Methylene blue (MB) and chlorpromazine (CP) reduced the fluorescence of native Complex II markedly. Since the analysis of the difference absorption spectra declared that MB and CP were intercalated without release of bound AO, the interacting MB and CP were considered to weaken the interaction between AO and DNA bases, that made AO more fluorescent. Free radical (CP·) of CP was prepared by a new method using H₂O₂, peroxidase, and ascorbic acid. Intercalated CP· showed a much stronger quenching effect on Complex II, indicating that unpaired electron spin contained in the costacking unit between CP· and DNA bases might affect the fluorescence of the adjacent AO molecule by paramagnetic perturbation.     

Molecular Complexes of acridine orange and nucleosides

Summary The addition of various nucleosides to the aqueous AO solution brings about the red shift of the absorption band of AO monomer and the enhancement of the AO fluorescence emission. These phenomena are attributable to the formation of a kind of molecular complex between AO monomer and nucleoside.The absorption and fluorescence characteristics and their thermal behaviours enable us to determine the association constant and the binding energy. The binding energy of AO with purines is larger than that with pyrimidines, and the association constant between AO and the deoxyribonucleoside is larger than that between AO and the ribonucleoside. For the molecular complexes dealt with, the face-to-face arrangement of AO and nucleoside, linking of AO with sugar by hydrogen bridge, may be more preferential than the side-by-side arrangement with the direct linkage between AO and nucleic acid base by hydrogen bonding. The Van der Waals-London interactions may be one of the essential factors for the binding in these molecular complexes.The association constant and the binding energy for AO-DNA and -RNA systems were also determined. The magnitude of these quantities seems to reflect the difference in the structure of these nucleic acids. The rather open structure of RNA compared with DNA is in favour of affinity with AO and gives the larger association constant than that for AO-DNA. The binding energy is somewhat larger for AO-DNA complex than for AO-RNA complex, probably due to the structural difference of the base arrangement; the stacked base pairs for DNA and the stacked bases for RNA.This may explain the selective degradation [12] of guanine photo-sensitized by dyes either in the free state or when incorporated to DNA or RNA, as discussed elsewhere.     

Heterogeneity of binding sites of proflavin on DNA

The desorption and melting with temperature of proflavine–DNA complexes has been studied by spectrophotometry and spectrofluorometry. Two methods are described to determine at each temperature the concentration of free and bound dye. The first one is based on the quenching of fluorescence of the free dye by the iodine ion, the second on fluorescence polarization measurements. It is shown that the sites where the bound dye fluoresces are thermally less stable than those where it is quenched, in such a way that a redistribution of the dye between the two types of sites occurs at intermediate temperatures, leading to a drop in the total fluorescence. This confirms the nature of the “emitting” sites which correspond to AT-rich region, while “quenched” sites correspond to GC-rich region. The first have a larger binding constant at room temperature, but only the latter are stabilized by dye intercalation. The desorption and melting have also been followed through the relative changes of absorption. The curves obtained at different wavelengths are not superimposed which is at variance with what is observed with complexes of proflavine with poly dAT and poly dG.dC. The beginning of the desorption process corresponds to minor variations at 445 nm, the maximum of absorption of the free dye, but large changes occur at 460 nm, the maximum of the difference spectrum of the complexes proflavine–poly dAT and proflavine-poly dG.dC. The spreading of the melting curves for different wave lengths must therefore reflect the dependence of the absorption spectra of the dye on the nature of the neighboring bases. However, the action spectrum of the fluorescence, which gives the absorption spectrum of the “emitting” sites only, is identical with the total absorption spectrum of the bound dye.     

Spectroscopic and computational approaches to unravel the mode of binding between a isoflavone,biochanin-A and calf thymus DNA

In the present study, attempt was made to explore the interaction between biochanin-A (BioA) and calf thymus DNA (ctDNA) by employing fluorescence spectroscopy, absorption spectroscopy, circular dichroism (CD), DNA melting studies, viscosity measurements, and molecular modeling methods. A well-known fluorescence probe, acridine orange (AO) was used in the present study in order to enhance the emission intensity of weakly fluorescent ctDNA. Quenching in emission intensity of ctDNA-AO system was observed in the presence of different concentrations of BioA, suggesting that BioA has interacted with ctDNA. The hyperchromic effect observed upon the addition of BioA in the absorption spectra of ctDNA-AO without any shift in its absorption maximum revealed that BioA was bound to ctDNA through groove mode of binding. Further the groove mode of binding of BioA to ctDNA was confirmed by DNA melting studies, viscosity measurements, and molecular docking studies. The results of fluorescence measurements that were carried out at different temperature indicated that the BioA has quenched the emission intensity of ctDNA-AO through static mode of quenching mechanism. Thermodynamic parameters revealed that the BioA-ctDNA-AO system was stabilized by van der Waals forces and hydrogen bonding. The effect of binding of BioA on the conformation of ctDNA was examined by circular dichroism studies.     

Stacking-unstacking dynamics of oligodeoxynucleotide trimers

The structure and dynamics of DNA trimers are experimentally assessed using the fluorescent purine analogue 2-aminopurine (2AP), incorporating 2AP between purine and pyrimidine bases to form 5'dXp2APpY3' molecules. Circular dichroism and fluorescence quenching of the 2AP show that the bases are stacked; at the same time, fluorescence decay lifetimes are heterogeneous, indicative of conformational sampling. 2AP does not exhibit the long fluorescence decay time characteristic of the free nucleoside, suggesting that its motions in the trimers bring it into proximity of the neighboring bases, resulting in efficient charge transfer and average fluorescence lifetimes on the order of 1-2 ns.     

Bertalanffy-like fluorescence staining with 3-dimethylamino-6-methoxyacridine

Three new acridine dyes, 3-dimethylamino-6-methoxyacridine 1, 3-amino-6-methoxyacridine 2 and 3-amino-7-methoxyacridine 3, have been prepared and tested as fluorochromes of LM- and HeLa-cells. The dyes are basic compounds (pKA: 1 8,76; 2 8,01; 3 7,65) and form cations in neutral or acidic aqueous solutions by addition of a proton to the aza-nitrogen atom of the heterocycle. The fluorochromes stain fixed LM- and HeLa-cells at pH = 6. The fluorescence shows metachromasy similar to the staining with acridine orange AO according to the technique of Bertalanffy. But there is less fading of the fluorescence. The dye 1 is the most suitable fluorochrome of the series. It was studied in detail. Using optimized staining conditions the fluorescence of the nucleus is yellow-green that of the cytoplasm and the nucleoli orange or brownish-red. Enzymatic digestion experiments show that the dye cations are bound to DNA in the nucleus and to RNA in the cytoplasm or nucleoli. The absorption and emission spectra of the stained cells have been studied by means of microspectrophotometry. The absorption spectra of the nucleus and the cytoplasm are very similar. The maximum of the long wave length absorption of both occurs at 21400 cm-1 (467 nm) with a shoulder at ca 20100 cm-1 (498 nm). The fluorescence spectra of nucleus and cytoplasm of metachromatically stained cells are different. The emission maximum of the cytoplasm and nucleoli, 16200 cm-1 (617 nm), is red-shifted relative to the maximum of the nucleus, 18200 cm-1 (549 nm). This shift causes the metachromatic fluorescence effect. In addition we studied the concentration dependence of the absorption and fluorescence spectra of the cation 1 in aqueous solution, pH = 6, in the concentration range 6 X 10(-6)-6 X 10(-4) M. Shape and maximum of the long wave length absorption and emission depend only slightly on the concentration: Mean value of absorption maximum ca 21500 cm-1 (465 nm), shoulder at ca 20300 cm-1 (493 nm), fluorescence maximum ca 18300 cm-1 (547 nm). With growing concentration diminishes the molar absorptivity. This decrease in absorptivity and isosbestic points in the absorption spectra indicate the formation of dimers with growing dye concentration. The absorption spectra of the metachromatically stained cells and of the dye in aqueous solution are very similar.(ABSTRACT TRUNCATED AT 400 WORDS)     

Conformational studies of Escherichia coli ribosomes with the use of acridine orange as a probe

The interaction of E. coli vacant ribosomes with acridine orange (AO) was studied, to obtain conformational information about rRNAs in ribosomes. Acridine orange binds to an RNA in two different modes: cooperative outside binding with stacking of bound AO's and intercalation between nucleotide bases. Free 16S and 23S rRNAs have almost identical affinities to AO. At 1 mM Mg2+, AO can achieve stacking binding on about 40% of rRNA phosphate groups. The number of stacking binding sites falls to about 1/3 in the 30S subunit in comparison with free 16S rRNA. In the 50S subunit, the number of stacking binding sites is only 1/5 in comparison with free 23S rRNA. Mg2+ ions are more inhibitory for the binding of AO to ribosomes than to free rRNAs. The strength of stacking binding appears to be more markedly reduced by Mg2+ in active ribosomes than in rRNAs. "Tight couple" 70S particles are less accessible for stacking binding than free subunits. The 30S subunits that have irreversibly lost the capability for 70S formation under low Mg2+ conditions have an affinity to AO that is very different from that of active 30S but similar to that of free rRNA, though the number of stacking binding sites is little changed by the inactivation. 70S and 30S ribosomes with stacking bound AO's have normal sedimentation constants, but the 50S subunits reversibly form aggregates.     

Studies on interaction between poly(L-lysine58, L-phenylalanine42) and deoxyribonucleic acids.

A random copolymer of 58% L-lysine and 42% L-phenylalanine, poly(Lys58Phe42), was used as a model protein for studying the role of phenylalanine residues in protein-DNA interaction. Complexes between this copolypeptide and DNA, made by direct mixing, were studied by absorbance, circular dichroism (CD), fluorescence, and thermal denaturation. Complex formation results in an increase in absorbance, and an enhancement, red-shift, and broadening of phenylalanine fluorescence. The fluorescence enhancement is opposite to the quenching observed when a tyrosine copolypeptide is bound to DNA (R. M. Santella and H.J. Li (1974), Biopolymers 13, 1909). The positive CD band of DNA near 275 nm is reduced and red-shifted by the binding of the phenylalanine copolypeptide to a greater extent than by the tyrosine copolypeptide. Thermal denaturation of the complexes in 2.5 times 10(-4) M EDTA (pH 8.0) shows three characteristic melting bands. For complexes with calf thymus DNA, free base pairs melt at Tm,I (47-49 degrees) and copolypeptide-bound base pairs show two melting bands (Tm,II at 73-75 degrees, and Tm,III at 88 -90 degrees). Similar thermal denaturation results have been observed for complexes with Micrococcus luteus DNA. The fluorecence intensity of the complexes is greatly increased when the temperature is raised to the Tm,II region. In addition to fluorescence measurements, the effects of increasing temperature on absorption and CD spectra of the complexes were also studied. Stacking interaction between the phenylalanine chromophore and DNA bases, either partial or full intercalation, is implicated by the experimental results. Several mechanisms are proposed to describe the reaction between the copolypeptide and DNA, and thermal denaturation of the complex.     

Discrete bathochromic shifts exhibited by fluorescein ligand bound to rabbit polyclonal anti-fluorescein Fab fragments

Eleven individual hyperimmune rabbit polyclonal anti-fluorescein Fab fragment preparations were resolved into heterogeneous subfractions based on differential dissociation times from a specific adsorbent. Four Fab subfractions (i.e., 0.1-, 1.0-, 10-, and 100-day elutions) that differed in affinity were characterized and classified according to the extent of the bathochromic shift in the absorption properties of antibody-bound fluorescein ligand. Absorption maxima of bound fluorescein were shifted in all cases to two distinct narrow ranges, namely, 505 to 507 nm or 518 to 520 nm relative to 491 nm for free fluorescein. There was no direct correlation between the two spectral shift populations and antibody affinity, fluorescence polarization, fluorescence quenching, or fluorescence lifetimes of bound ligand. Fluorescence emission maxima varied with the bathochromic shift range. Bound fluorescein ligand, with absorption maxima of 505 to 507 nm and 518 to 520 nm showed fluorescence emission maxima of 519 to 520 nm and 535 nm, respectively. The two spectral shift ranges differed by 14 to 15 nm and/or energies of 1.5 kcal mol^–1 relative to each other and to the absorption maximum for free fluorescein. Spectral effects on the antibody-bound ligand were discussed relative to solvent-water studies and the atomic structure of a high-affinity liganded anti-fluorescein active site.     

Actinomycin D and 7-aminoactinomycin D binding to single-stranded DNA

The potent RNA polymerase inhibitors actinomycin D and 7-aminoactinomycin D are shown to bind to single-stranded DNAs. The binding occurs with particular DNA sequences containing guanine residues and is characterized by hypochromic UV absorption changes similar to those observed in interactions of the drugs with double-stranded duplex DNAs. The most striking feature of the binding is the dramatic (ca. 37-fold) enhancement in fluorescence that occurs when the 7-aminoactinomycin is bound to certain single-stranded DNAs. This fluorescence of the complex is also characterized by a 40-nm hypsochromic shift in the emission spectrum of the drug and an increase in the emission anisotropy relative to the free drug or the drug bound to calf thymus DNA. The fluorescence lifetimes change in the presence of the single-stranded DNA in a manner compatible with the intensity difference. Thus, there is an increase in the fraction of the emission corresponding to a 2-ns lifetime component compared to the predominant approximately 0.5-ns lifetime of the free drug. The 7-aminoactinomycin D comigrates in polyacrylamide gels with the single-stranded DNAs, and the fluorescence of the bound drug can be visualized by excitation with 540-nm light. The binding interactions are characterized by association constants of 2.0 x 10(6) to 1.1 x 10(7) M-1.     

Cytochrome c interaction with membranes. Absorption and emission spectra and binding characteristics of iron-free cytochrome c.

A cytochrome c derivative from which iron is removed has been prepared and characterized. Several lines of evidence indicate that native and porphyrin cytochrome c have similar conformations: they have similar elution characteristics on Sephadex gel chromatography; in both proteins the tryptophan fluorescence is quenched and the pK values of protonation of the porphyrin are identical. Porphyrin cytochrome c does not substitute for native cytochrome c in either the oxidase reaction or in restoring electron transport in cytochrome-c-depleted mitochondria. It does however competitively inhibit native cytochrome c in these reactions, the Ki for inhibition being larger than the Km for reaction. The absorption and emission spectra, and the polarized excitation spectrum of the porphyrin cytochrome c are characteristic of free base porphyrin. The absence of fluorescence quenching of porphyrin cytochrome c when the protein is bound to cytochrome oxidase suggests that heme to heme distance between these proteins is larger than 0.5 to 0.9 nm depending upon orientation. Binding of the porphyrin cytochrome c to phospholipids or to mitochondria increases the fluorescence polarization of a positively polarized absorption band, which indicates that the bound form of the protein does not rotate freely within the time scale of relaxation from the excited state.     

Complexes produced by associated forms of porphyrin bound with hydrophobic-hydrophilic copolymer and transition metal ions

Properties of protonated dimeric forms of meso-tetraphenylporphine (TPP) and meso-tetra(p-aminophenyl)porphine (TAPP) bound with copolymer and also complexes produced by associated TAPP bound with copolymer, Mn2+, and Fe3+ are investigated by absorption, luminescence, and Raman spectroscopy. According to absorption spectra of protonated dimers of TPP, three dimeric forms of the porphyrin are observed in the ground state. However, selective excitation of these forms according to the fluorescence spectra reveals only two dimeric forms in the excited state. In contrast, similar selective excitation of TAPP bound with copolymer in aqueous-dioxane solution results in weak changes in the fluorescence spectra, nevertheless, there is strong interaction between porphyrin and macromolecular carboxyl groups in the ground state. In the case of the formation of the complexes between associated TAPP bound with copolymer, Mn2+ and Fe3+, a new band in the near IR region with a maximum at 840 nm is built up in the fluorescence spectrum. However, this near IR emission is completely quenched when new strong vibrational bands at approximately 1800 and 1900 cm-1 are revealed in the resonance Raman spectra of the complexes. The observed effects are explained in terms of direct participation of water molecules involved in the water-porphyrin dimeric complex in the processes of transformation of excitation energy. The involvement of water in this dimeric complex can lead to redistribution of flows of the energy degradation when transition metal ions play a role of the agent which enhances the trapping properties of the porphyrin-metal-ions complexes.     

Decay-associated emission spectra and other spectral evidence for the physical intercalation of 7,8-dihydroxy-7,8-dihydrobenzo[a]pyrene into DNA

A benzo[a]pyrene derivative, 7,8-dihydroxy-7,8-dihydrobenzo[a]pyrene, forms physical complexes with DNA. The measured absorption spectrum of the hydrocarbon in the complex is shifted approximately 10 nm to the red and the fluorescence emission spectrum is red-shifted approximately 6 nm, characteristic of a physical intercalation complex. The decay-associated emission spectra of the hydrocarbon in the presence of DNA have been measured, thus providing a new technique to obtain information about the DNA binding sites. The decay-associated emission spectra of the free and bound hydrocarbons were obtained by deconvoluting the time-dependent emission at several wavelengths. Stern-Volmer plots with iodide and silver ions as quenchers suggest that at least one set of binding sites for the formation of a physical intercalation complex between the benzo[a]pyrene derivative and DNA is at guanine sites in the biopolymer.     

Photophysics of tryptophan in bacteriophage T4 lysozymes

Bacteriophage T4 lysozyme contains three tryptophan residues in distinct environments. Lysozymes with one or two of these residues replaced by tyrosine are used to characterize the photophysics of tryptophan in these individual sites. The fluorescence spectra, average lifetimes, and quantum yields of these three single-tryptophan variants are understandable in terms of the neighboring residues. The emission spectra and radiative lifetimes are found to be the same for all three species while the quantum yield and decay kinetics are quite distinct. The variation of the average nonradiative rate constant is correlated with neighboring quenching groups. Quenching by I- correlates with exposure of the tryptophan residue based on the crystal structure. Complex behavior is observed for the time dependence of the fluorescence decay in all three cases, including that of the immobile tryptophan-138 residue. The complexity of the fluorescence decay is ascribed to heterogeneity in the nonradiative rate constant among microstates. Energy transfer between tryptophan residues is inferred to occur from comparison of the quantum yields of the two-tryptophan and single-tryptophan proteins and is discussed in terms of the F?rster mechanism.     

Acridine orange interaction with DNA: Effect of ionic strength

BackgroundThe study of acridine orange (AO) spectral characteristics and the quenching of its singlet and triplet excited states by TEMPO radical at its binding to DNA in the function of the DNA concentration and in the absence and presence of NaCl is reported.MethodsThe study was performed using steady-state and time resolved optical absorption and florescence, fluorescence correlation spectroscopy and resonant light scattering techniques.ResultsThe presence of different species in equilibrium: AO monomers and aggregates bound to DNA, has been demonstrated, their relative content depending on the DNA and the AO concentrations. At high DNA concentration the AO monomers are protected against the contact with other molecules, thus reducing the AO excited state quenching. The addition of NaCl reduces the AO binding constant to DNA, thus reducing the AO and DNA aggregation.ConclusionsThe interaction of AO with DNA is a complex process, including aggregation and disaggregation of both components. This modifies the AO excited state characteristics and AO accessibility to other molecules. The salt reduces the DNA effects on the AO excited state characteristics thus attenuating its effects on the AO efficacy in applications.General significanceThis study demonstrates that the interaction of photosensitizers with DNA, depending on their relative concentrations, can both decrease and increase the photosensitizer efficacy in applications. The salt is able to attenuate these effects.     

Acridine orange distribution and fluorescence spectra in myoblasts and single muscle fibers

Acridine orange (AO) fluorescence spectra in nuclei and cytoplasm of living myoblasts L6J1 and frog single muscle fibers have been studied using spectral scanning system of Leica TCS SL confocal microscope. AO fluorescence spectra in salt solutions dependent on free AO concentrations or in complex with DNA have also been obtained. Myoblast nuclei fluoresced in the green spectral region with maximum at about 530 nm; nucleoli had the brightest fluorescence. The fluorescence of nuclear chromatin was not uniform. Similar fluorescence of nuclei and nucleoli was observed in frog single muscle fibers. Uniform, weak, green fluorescence was observed in the myoblast cytoplasm. In the sarcoplasm of muscle fibers, AO green fluorescence was seen in A discs. In the cytoplasm of myoblasts and muscle fibers stained with AO, different red, yellow, and green fluorescent granules, which were acidic organelles, were visualized. The comparison of AO fluorescence spectra in living cells with AO fluorescence spectra in buffer solutions with different AO concentrations and AO in complex with DNA enables the estimation of the AO concentration in acidic granules. It is important for the evaluation of these cellular organelles functions in intracellular transport, adaptation, and apoptosis, as well as in a number of pathological processes.     

7-Amino-actinomycin D as a cytochemical probe. I. Spectral properties.

The optical absorption and fluorescence characteristics of 7-animo-actinomycin D were determined to evaluate its potential as a fluorescent cytochemical probe. At pH 7.0, the absorption maximum and fluorescence excitation maximum are both at 503 nm; the fluorescence emission is at 675 nm. When this compound forms complexes with DNA in solution, the absorption and fluorescence excitation maxima shift to 543 nm and the fluorescence emission shifts to 655 nm. The fluorescence quantum yield is 0.016 for 7-amino-actinomycin D free in solution and 0.01-0.02 for complexes with native DNA. The 7-amino-actinomycin D also exhibits fluorescence shifts characteristic of binding when put into solution with poly(dG-dC) poly(dG-dC), but not with poly(dI-dC) poly(dI-dC). The spectral characteristics are the same at pH 7.0 whether the solvent is 0.01 M PO4 with 0.0001 M EDTA or Earle's salts with 0.025 M N-2-hydroxyethylpiperazine-N1-2-ethanesulfonic acid.     

Antibody-hapten interactions: circular and linear polarization of the fluorescence of dansyl bound to anti-dansyl antibodies

The fluorescence spectra of several dansyl derivatives (dansylamide, ?-N-dansyl-l-lysine, dansyl-l-alanine, and α-N-dansyl-l-alanine amide) bound to anti-dansyl antibodics (induced by an α-N-dansyl-poly d,l-alanine-poly l-lysine conjugate) are shifted by about 60 nm to the blue, and the quantum yields are markedly enhanced, compared to their respective fluorescence properties in water. The light emitted by the bound haptens is partly circularly polarized, reflecting the asymmetry induced in the bound chromophores by the antibody combining site. In contradistinction, the fluorescence spectrum of 1-dansyl-2-alanine diaminoethane bound to anti-alanine antibodies is similar to that of the free fluorophore in water and lacks circular polarization. These results imply that in this case the fluorophore of the hapten protrudes out of the site into the aqueous solvent. No circular dichroism is observed in the 300 to 400 nm region for the dansyl-anti-dansyl complex. Thus a change in the mode of interaction between the chromophore and its binding site takes place upon electronic excitation. The heterogeneity of the antibody binding sites is expressed by the dependence of the circular polarization of fluorescence on excitation wavelength. Differences in the circular polarization of luminescence were also observed when the residues attached to the dansyl group have been varied. This may reflect differences in the alignment of the fluorophore within the binding sites for the different dansyl derivatives.The linear polarization of dansylamide dissolved in glycerol is not constant across the emission band, indicating that the transition dipole moments related to the various vibronic states do not have the same spatial directions. Vibronic mixing of the emitting excited state with higher electronic states is thus indicated. Dansyl-l-alanine bound to anti-dansyl antibodies exhibitsan even more pronounced variation of the linear polarization across the emission band. In this case, the dependence of the linear polarization of the emitted light on excitation wavelength is anomalous, which is again a reflection of the heterogeneity of the population of the antibody molecules. The implications of these results to the studies of the fluorescence polarization of dansyl-protein complexes are discussed.     

De-intercalation of ethidium bromide and acridine orange by xanthine derivatives and their modulatory effect on anticancer agents: a study of DNA-directed toxicity enlightened by time correlated single photon counting

Time Correlated Single Photon Counting (TCSPC) was used for the first time to analyze the effect/changes in the mode of intercalation of ethidium bromide (EtBr) and acridine orange (AO) to calf thymus DNA brought about due to interaction of naturally occurring methylxanthines such as theophylline (X1), theobromine (X2) and caffeine (X3). UV absorption and fluorescence studies were also carried to observe the behaviour of these xanthines on the modulation of the binding mode of anticancer agents (cisplatin, novantrone, and actinomycin D) and certain intercalating dyes (EtBr and AO) to DNA. In TCSPC analysis we found that when the concentration of the drugs (X1, X2 and X3) increased from 0.025 mM to 2 mM i.e. P/D 2.4 to P/D 0.03 reduction in intercalation of EtBr and AO was observed, suggesting that xanthine derivatives could play very important role in reducing the DNA-directed toxicity in a dose dependent manner. In TCSPC, the amplitude of smaller lifetime component A(1) and higher lifetime component A(2) are attributed to free and intercalated dye concentration and their variation could indicate the process of intercalation or reduced intercalation of EtBr and AO by xanthine derivatives. We found that at the maximum drug concentration the smaller lifetime component A(1) was increased by 7-8% and 17-37% in EtBr and AO intercalated complex respectively. Also the changes in lifetime and fluorescence decay profile were observed for the DNA-intercalated dyes before and after treatment with xanthines. Especially, at maximum P/D 0.03 the lifetime of DNA-intercalated EtBr and AO reduced by 1-2 ns. The present analysis reveals that xanthines are able to interact with free dyes and also with intercalated dyes, suggesting that when they interact with free dyes they might inhibit the further intercalation of dye molecules to DNA and the interaction with intercalated dyes might lead to displacement of the dyes resulting in de-intercalation. The results obtained from UV and fluorescence spectroscopy also support the present investigation of probable interaction of xanthines with the DNA damaging agents in modulating/reducing the DNA-directed toxicity.