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.     

Fluorescence lifetime analysis of DNA intercalated ethidium bromide and quenching by free dye

The fluorescence characteristics of ethidium bromide (Eb) complexed to calf thymus DNA have been examined using fluorescence lifetime analysis for a range of DNA (effective nucleotide concentration) to Eb molar ratios. Control of both temperature and ion concentration is necessary for reproducible analyses. Eb complexed to double stranded DNA has a maximum fluorescence lifetime of 23 ns and is easily distinguishable from a fluorescence lifetime value of 1.67 ns corresponding to unbound Eb. In a solution of calf thymus DNA containing excess Eb a binding equilibrium is reached, and this corresponds to one Eb molecule for every five nucleotides. With increasing amounts of unbound Eb, the fluorescence lifetime of the DNA-Eb complex decreases with a concomitant drop in the steady state fluorescence intensity, without a change in the amount of Eb bound to DNA. It is concluded that unbound Eb, acting via a quenching mechanism, shortens the fluorescence lifetime of bound Eb and consequently decreases the overall fluorescence intensity. This means that a different approach is necessary: time-resolved fluorescence spectroscopy directly distinguishes between a decrease in fluorescence intensity due to quenching by an excess of unbound Eb from that due to a decrease in Eb binding to double-stranded DNA. These studies suggest that techniques which measure total steady state fluorescence intensity of bound Eb in order to infer relative amounts of double-stranded DNA must be interpreted with caution. For such assays to be valid it is essential that no unbound Eb be present; otherwise a variable correction factor is required to account for unbound Eb.     

The possible role of electron-transfer complexes in the antitumour action of amsacrine analogues

Amsacrine is a DNA intercalating agent which is active against a number of tumours in mice and is used for the treatment of leukaemia in humans. In its DNA-bound form, amsacrine efficiently quenches the fluorescence of ethidium. Fluorescence lifetime studies demonstrate two populations of DNA-bound ethidium. The first, whose fluorescence lifetime is constant at approx. 3 ns and whose proportion increases with increasing amsacrine binding ratio, may comprise molecules bound in close proximity to amsacrine. The second, whose fluorescence lifetime is longer and variable (10-24 ns) and whose proportion decreases with increasing amsacrine binding ratio, may comprise molecules three or more base-pairs away from ethidium. Studies with a number of derivatives of 9-anilinoacridine containing different anilino substituents suggest that the observed wide variation in quenching capacity is correlated with the magnitude of the substituent dipole moment in a particular direction. Consideration of the geometry of the DNA-binding complex indicates that the negative pole of a dipole established in the anilino ring is directed towards a positively charged site on the ethidium molecule. Quenching of ethidium fluorescence may therefore occur where an electron-transfer complex has formed between ethidium and amsacrine molecules. To ascertain whether electron-transfer complex formation is biologically important in the amsacrine series, ethidium quenching has been quantitated and compared with activity against a transplantable neoplasm in mice, the Lewis lung carcinoma. Compounds which strongly quench ethidium fluorescence are in general highly active antitumour agents. The results are discussed in terms of a model where amsacrine has both a DNA-binding and a protein-binding domain, the latter possibly interacting by formation of an electron-transfer complex. The most likely protein-binding domain is on the enzyme topoisomerase II, the target for its cytotoxic activity.     

Distance between the agonist and noncompetitive inhibitor sites on the nicotinic acetylcholine receptor

The nicotinic acetylcholine receptor possesses an agonist binding site on each of the two alpha-subunits and an allosterically coupled noncompetitive inhibitor (NCI) site. The spatial relationships between these sites have been determined by fluorescence energy transfer employing lifetime and steady-state techniques with two donor-acceptor pairs. 6-(5-Dimethylaminonaphthalene-1-sulfonamido)hexanoic acid-beta-(N-trimethylammonium)ethyl ester (dansyl-C6-choline, an agonist) and bis(choline)-N-(4-nitrobenzo-2-oxa-1,3-diazol-7-yl)-iminodiprop rionate (BCNI, a competitive antagonist) were employed as energy donors bound to the agonist sites. Ethidium was employed as a specific probe of the NCI site and served as the energy acceptor for both donors. Under steady-state conditions, energy transfer was measured by monitoring BCNI fluorescence as a function of occupancy of ethidium. Changes in acceptor occupancy were achieved by titrating acetylcholine receptor-donor-acceptor complexes with phencyclidine, a nonfluorescent NCI ligand. Extrapolation of the data to 100% acceptor occupancy yielded a transfer efficiency of 38% for the BCNI-ethidium pair. In the second method, the transfer efficiency of the dansyl-C6-choline-ethidium pair was determined by analysis of the reduction of the donor-excited state fluorescence lifetime. The nanosecond decay rates for dansyl-C6-choline measured in the presence of phencyclidine are characterized by two lifetimes (tau 1 = 6.7; tau 2 = 17.1 ns) with an amplitude ratio, alpha 1/alpha 2 = 2.3. In the presence of ethidium, the two lifetimes were proportionally diminished while retaining a comparable ratio of amplitudes. Displacement of ethidium from the NCI site by phencyclidine restored the two lifetimes to their original values. These data indicate that the donors bound to the two agonist sites transferred energy with similar efficiencies to the acceptor. Thus, the lifetime data suggest that the NCI site is approximately equidistant from each of the agonist sites. The corrected efficiency of donor quenching by this method was 34%, a value in close accord with the steady-state measurements. The distance between the agonist sites and the NCI site was calculated to be between 21-35 A for the BCNI/ethidium pair and 22-40 A for the dansyl-C6-choline/ethidium pair. Consideration of these distances with respect to the molecular dimensions of the receptor and location of the agonist sites suggests a location for the NCI site near the ion channel at the extracellular surface of the membrane bilayer.     

Influence of the triplet excited state on the photobleaching kinetics of fluorescein in microscopy.

The investigation in this report aimed at providing photophysical evidence that the long-lived triplet excited state plays an important role in the non-single-exponential photobleaching kinetics of fluorescein in microscopy. Experiments demonstrated that a thiol-containing reducing agent, mercaptoethylamine (MEA or cysteamine), was the most effective, among other commonly known radical quenchers or singlet oxygen scavengers, in suppressing photobleaching of fluorescein while not reducing the fluorescence quantum yield. The protective effect against photobleaching of fluorescein in the bound state was also found in microscopy. The antibleaching effect of MEA let to a series of experiments using time-delayed fluorescence spectroscopy and nanosecond laser flash photolysis. The combined results showed that MEA directly quenched the triplet excited state and the semioxidized radical form of fluorescein without affecting the singlet excited state. The triplet lifetime of fluorescein was reduced upon adding MEA. It demonstrated that photobleaching of fluorescein in microscopy is related to the accumulation of the long-lived triplet excited state of fluorescein and that by quenching the triplet excited state and the semioxidized form of fluorescein to restore the dye molecules to the singlet ground state, photobleaching can be reduced.     

Synthesis and photophysical properties of zinc myoglobin appending an ethidium ion as a DNA intercalator

In order to elucidate the intramolecular photoinduced electron-transfer or energy-transfer mechanisms of the zinc myoglobin (ZnMb) dyad and to construct a photoreaction system within a Mb–DNA complex, we newly prepared ZnMb appending an ethidium ion (Et⁺). The steady-state fluorescence of ZnMb–Et⁺ at 600 nm and its lifetime (2.2 ns) indicate that the excited singlet state of ¹(ZnMb)* is not quenched by the Et⁺ moiety, whereas the lifetime of the excited triplet state of ³(ZnMb)*–Et⁺ was shorter (τ = 4.3 ms) than those of ZnMb and the intermolecular (ZnMb + ethidium) system. Upon photoirradiation of Et⁺, fluorescence studies indicated the intramolecular quenching reactions from the excited singlet state, ¹(Et⁺)*, to ZnMb, the process of which is likely the photoinduced energy-transfer reaction via a through-space mechanism. We also demonstrate the photophysical and spectroscopic properties of ZnMb–Et⁺ in the presence of calf thymus (CT) DNA. The changes in the absorption and fluorescence spectra of ZnMb–Et⁺ on the addition of CT-DNA up to 15 equiv were very small, indicating that there are no major changes in the heme pocket. However, we observed a longer lifetime of ³(ZnMb)*–Et⁺ in the presence of CT-DNA (τ = 5.3 ms) by single flash photolysis. This was induced by noncovalent interactions between Et⁺ and CT-DNA, followed by a conformational change of Et⁺ at the surface of ZnMb, where the donor–acceptor distance was probably elongated by CT-DNA. The synthetic manipulation at the Mb surface, by using a DNA intercalator coupled with photoinduced reaction, may provide a sensitive transient signal for DNA and valuable information to construct new Mb–DNA complex. Electronic supplementary material The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

The effect of oxygen on the amplitude of photodriven electron transfer across the lipid bilayer-water interface.

The surprisingly small effect of oxygen on photoelectron transfer in pigmented lipid bilayers is traced to a short lifetime of the excited states. Decreasing the oxygen concentration by greater than 100-fold decreases the half saturating concentration of acceptor by only threefold and has no effect on the maximum photovoltage observed at acceptor saturation. This holds true for both magnesium octaethylporphyrin and chlorophyll with both ferricyanide and methyl viologen as acceptors. Since oxygen quenches excited states at near the encounter limit, the lifetime of reactive state must be short, less than 100 ns. About 100-fold higher concentrations of acceptor are required to quench the fluorescence (in liposomes) than to saturate the photoeffect. Thus the reactive state is most likely the triplet. The short life of the excited state is caused by concentration quenching, i.e., their reaction with ground state molecules. The increase of photovoltage with increasing pigment concentration shows that this quenching in a condensed form of the pigment produces ions that lead to the observed photovoltage by interfacial reaction of the anion with acceptor.     

Optical studies of complexes of quinacrine with DNA and chromatin: implications for the fluorescence of cytological chromosome preparations

The fluorescence and circular dichroism of quinacrine complexed with nucleic acids and chromatin were measured to estimate the relative magnitudes of factors influencing the fluorescence banding patterns of chromosomes stained with quinacrine or quinacrine mustard. DNA base composition can influence quinacrine fluorescence in at least two ways. The major effect, evident at low ratios of quinacrine to DNA, is a quenching of dye fluorescence, correlating with G-C composition. This may occur largely prior to relaxation of excited dye molecules. At higher dye/DNA saturations, which might exist in cytological chromosome preparations stained with high concentrations of quinacrine, energy transfer between dye molecules converts dyes bound near G-C base pairs into energy sinks. In contrast to its influence on quinacrine fluorescence, DNA base composition has very little effect on either quinacrine binding affinity or the circular dichroism of bound quinacrine molecules. The synthetic polynucleotides poly(dA-dT) and poly(dA)-poly(dT) have a similar effect on quinacrine fluorescence, but differ markedly in their affinity for quinacrine and in the circular dichroism changes associated with quinacrine binding. Quinacrine fluorescence intensity and lifetime are slightly less when bound to calf thymus chromatin than when bound to calf thymus DNA, and minor differences in circular dichroism between these complexes are observed. Chromosomal proteins probably affect the fluorescence of chromosomes stained with quinacrine, although this effect appears to be much less than that due to variations in DNA base composition. The fluorescence of cytological chromosome preparations may also be influenced by fixation effects and macroscopic variations in chromosome coiling.     

利用荧光寿命变化定量分子内和分子间相互作用的方法

荧光寿命是指荧光分子在回到基态前在激发态停留的平均时间.本文发展了基于荧光寿命测量来定量分子内和分子间相互作用的方法:通过G碱基猝灭对于荧光寿命的影响定量DNA二级结构的形成;通过荧光共振能量传递(FRET)中荧光寿命的变化来定量分子间的相互作用.第一种方法巧妙利用了G碱基会猝灭临近的染料分子的性质,结合荧光寿命的变化,可以判断DNA二级结构的形成以及形成的比率. FRET是用于研究生物分子相互作用的一个重要手段.传统的FRET方法主要是基于强度的变化,但这种变化容易受到荧光表达水平变动、样品中分子扩散以及荧光串色的影响,因此经常存在着实验比较复杂和重复性差的问题.而基于荧光寿命的FRET研究则可以很好地克服上述缺点.通过检测供体荧光寿命的变化,我们能够方便快捷地判断是否发生FRET,并通过建立系统的数据分析方法,得到FRET的效率以及分子之间相互作用的信息.     

Fluorescence decay and quantum yield characteristics of acridine orange and proflavine bound to DNA

Fluorescence properties (quantum yield, decay curve, lifetime and polarization) of acridine orange and proflavine bound to DNA were examined as a function of nucleotide to dye (P/D) ratio. First, mean fluoiescence lifetimes were determined by the phase-shift measurements. The lifetime and quantum yield of acridine orange increased in a parallel fashion with increasing P/D ratio. There was no parallel relation between the lifetime and quantum yield for proflavine; the lifetime showed a minimum around P/D = 10. Next, fluorescence decay curves were measured by the monophoton counting technique and analyzed with the aid of the method of moments and the Laplace transform method. The results showed that the fluorescence decay of bound acridine orange was exponential above P/D = 10. On the other hand, the decay of bound proflavine was exponential above P/D = 100, but markedly deviated from exponentiality with decreasing P/D ratio. The results of fluorescence polarization suggested that this phenomenon is the result of Förster energy transfer between proflavine molecules bound to the fluorescent site (AT pair) and bound to the quenching site (GC pair). Critical transfer distances were 26-4 and 37.0 Å, respectively, for bound proflavine and acridine orange.     

Binding of ethidium to the nucleosome core particle. 2. Internal and external binding modes

We have previously reported that the binding of ethidium bromide to the nucleosome core particle results in a stepwise dissociation of the structure which involves the initial release of one copy each of H2A and H2B (McMurray & van Holde, 1986). In this report, we have examined the absorbance and fluorescence properties of intercalated and outside bound forms of ethidium bromide. From these properties, we have measured the extent of external, electrostatic binding of the dye versus internal, intercalation binding to the core particle, free from contribution by linker DNA. We have established that dissociation is induced by the intercalation mode of binding to DNA within the core particle DNA, and not by binding to the histones or by nonintercalative binding to DNA. The covalent binding of [3H]-8-azidoethidium to the core particle clearly shows that less than 1.0 adduct is formed per histone octamer over a wide range of input ratios. Simultaneously, analyses of steady-state fluorescence enhancement and fluorescence lifetime data from bound ethidium complexes demonstrate extensive intercalation binding. Combined analyses from steady-state fluorescence intensity with equilibrium dialysis or fluorescence lifetime data revealed that dissociation began when approximately 14 ethidium molecules are bound by intercalation to each core particle and less than 1.0 nonintercalated ion pair was formed per core particle.     

Analysis of hydride transfer and cofactor fluorescence decay in mutants of dihydrofolate reductase: possible evidence for participation of enzyme molecular motions in catalysis.

A remarkable correlation has been discovered between fluorescence lifetimes of bound NADPH and rates of hydride transfer among mutants of dihydrofolate reductase (DHFR) from Escherichia coli. Rates of hydride transfer from NADPH to dihydrofolate change by a factor of 1,000 for the series of mutant enzymes. Since binding constants for the initial complex between coenzyme and DHFR change by only a factor of 10, the major portion of the change in hydride transfer must be attributed to losses in transition-state stabilization. The time course of fluorescence decay for NADPH bound to DHFR is biphasic. Lifetimes ranging from 0.3 to 0.5 ns are attributed to a solvent-exposed dihydronicotinamide conformation of bound coenzyme which is presumably not active in catalysis, while decay times (tau 2) in the range of 1.3 to 2.3 ns are assigned to a more tightly bound species of NADPH in which dihydronicotinamide is sequestered from solvent. It is this slower component that is of interest. Ternary complexes with three different inhibitors, methotrexate, 5-deazafolate, and trimethoprim, were investigated, along with the holoenzyme complex; 3-acetylNADPH was also investigated. Fluorescence polarization decay, excitation polarization spectra, the temperature variation of fluorescence lifetimes, fluorescence amplitudes, and wavelength of absorbance maxima were measured. We suggest that dynamic quenching or internal conversion promotes decay of the excited state in NADPH-DHFR. When rates of hydride transfer are plotted against the fluorescence lifetime (tau 2) of tightly bound NADPH, an unusual correlation is observed. The fluorescence lifetime becomes longer as the rate of catalysis decreases for most mutants studied. However, the fluorescence lifetime is unchanged for those mutations that principally alter the binding of dihydrofolate while leaving most dihydronicotinamide interactions relatively undisturbed. The data are interpreted in terms of possible dynamic motions of a flexible loop region in DHFR which closes over both substrate and coenzyme binding sites. These motions could lead to faster rates of fluorescence decay in holoenzyme complexes and, when correlated over time, may be involved in other motions which give rise to enhanced rates of catalysis in DHFR.     

Probing structure and dynamics of DNA with 2-aminopurine: effects of local environment on fluorescence

2-Aminopurine (2AP) is an analogue of adenine that has been utilized widely as a fluorescence probe of protein-induced local conformational changes in DNA. Within a DNA strand, this fluorophore demonstrates characteristic decreases in quantum yield and emission decay lifetime that vary sensitively with base sequence, temperature, and helix conformation but that are accompanied by only small changes in emission wavelength. However, the molecular interactions that give rise to these spectroscopic changes have not been established. To develop a molecular model for interpreting the fluorescence measurements, we have investigated the effects of environmental polarity, hydrogen bonding, and the purine and pyrimidine bases of DNA on the emission energy, quantum yield, and intensity decay kinetics of 2AP in simple model systems. The effects of environmental polarity were examined in a series of solvents of varying dielectric constant, and hydrogen bonding was investigated in binary mixtures of water with 1,4-dioxane or N,N-dimethylformamide (DMF). The effects of the purine and pyrimidine bases were studied by titrating 2AP deoxyriboside (d2AP) with the nucleosides adenosine (rA), cytidine (rC), guanosine (rG), and deoxythymidine (dT), and the nucleoside triphosphates ATP and GTP in neutral aqueous solution. The nucleosides and NTPs each quench the fluorescence of d2AP by a combination of static (affecting only the quantum yield) and dynamic (affecting both the quantum yield and the lifetime, proportionately) mechanisms. The peak wavelength and shape of the emission spectrum are not altered by either of these effects. The static quenching is saturable and has half-maximal effect at approximately 20 mM nucleoside or NTP, consistent with an aromatic stacking interaction. The rate constant for dynamic quenching is near the diffusion limit for collisional interaction (k(q) approximately 2 x 10(9) M(-1) s(-1)). Neither of these effects varies significantly between the various nucleosides and NTPs studied. In contrast, hydrogen bonding with water was observed to have a negligible effect on the emission wavelength, fluorescence quantum yield, or lifetime of 2AP in either dioxane or DMF. In nonpolar solvents, the fluorescence lifetime and quantum yield decrease dramatically, accompanied by significant shifts in the emission spectrum to shorter wavelengths. However, these effects of polarity do not coincide with the observed emission wavelength-independent quenching of 2AP fluorescence in DNA. Therefore, we conclude that the fluorescence quenching of 2AP in DNA arises from base stacking and collisions with neighboring bases only but is insensitive to base-pairing or other hydrogen bonding interactions. These results implicate both structural and dynamic properties of DNA in quenching of 2AP and constitute a simple model within which the fluorescence changes induced by protein-DNA binding or other perturbations may be interpreted.     

Photophysics of thionine dye in aqueous and liposome media in presence of different reducing agents.

The photoelectrochemical and spectral (both absorption and fluorescence) studies of thionine, a cationic phenothiazine dye, have been carried out in aqueous and phosphatidylcholine liposome media in the presence of different reducing agents, such as I(-), Br(-), Cl(-) and Fe(2+). The results show that the photovoltage generation from photoelectrochemical studies and Stern-Volmer quenching constant studied by fluorescence quenching support the photoinduced electron transfer from the reducing agent to the singlet excited thionine dye. Moreover, a good correlation between photovoltages/Stern-Volmer quenching constants vs. reduction potentials of the reducing agents also confirms the above electron transfer in the photoexcited state.     

Quinacrine: Spectroscopic properties and interactions with polynucleotides

The acridine dye quinacrine and its interactions with calf thymus DNA, poly(dA-dT) · poly (dA-dT), and poly (dG-dC) · poly(dG-dC) were studied by light absorption, linear dichroism, and fluorescence spectroscopy. The transition moments of quinacrine give rise to absorption bands polarized along the short axis (400–480-nm band), and the long axis (345-nm and 290-nm bands) of the molecule, respectively. Linear dichroism studies show that quinacrine intercalates into calf thymus DNA as well as into the polynucleotides, displaying fairly homogeneous binding to poly (dA-dT) · poly (dA-dT), but more than one type of intercalation site for calf thymus DNA and poly (dG-dC) · poly(dG-dC). Fluorescence spectroscopy shows that for free quinacrine the pK = 8.1 between the mono- and diprotonated states also remains unchanged in the excited state. Quinacrine bound to calf thymus DNA and polynucleotides exhibits light absorption typical for the intercalated diprotonated form. The fluorescence enhancement of quinacrine bound to poly (dA-dT) · poly(dA-dT) may be due to shielding from water interactions involving transient H-bond formation. The fluorescence quenching in poly(dG-dC) · poly(dG-dC) may be due to excited state electron transfer from guanine to quinacrine. © 1993 John Wiley & Sons, Inc.     

Far-red fluorescence: a direct spectroscopic marker for LHCII oligomer formation in non-photochemical quenching

Time-resolved fluorescence on oligomers of the main light-harvesting complex from higher plants indicate that in vitro oligomerization leads to the formation of a weakly coupled inter-trimer chlorophyll-chlorophyll (Chl) exciton state which converts in tens of ps into a state which is spectrally broad and has a strongly far-red enhanced fluorescence spectrum. Both its lifetime and spectrum show striking similarity with a 400ps fluorescence component appearing in intact leaves of Arabidopsis when non-photochemical quenching (NPQ) is induced. The fluorescence components with high far-red/red ratio are thus a characteristic marker for NPQ conditions in vivo. The far-red emitting state is shown to be an emissive Chl-Chl charge transfer state which plays a crucial part in the quenching.     

Strategies for choosing a deoxyribonucleic acid stain for flow cytometry of metaphase chromosomes.

Requirements for flow cytometry of metaphase chromosomes stained with three deoxyribonucleic acid (DNA)-specific fluorescent dyes--Hoechst 33258, Chromomycin A3, and ethidium bromide--are reviewed. Fluorescence properties of these three stains when bound to mitotic cells or to chromosomes in suspension are measured and compared with fluorescence properties when bound to DNA in solution. Conditions are given for high resolution flow cytometry of Chinese hamster chromosomes stained with each of the fluorophors, and histograms are presented that exhibit differences in relative peak position and area. Energy transfer fluorescence between two DNA stains is presented as a potentially useful new parameter for flow cytometry of chromosomes and is illustrated by fluorescence energy transfer from Chromomycin A3 to ethidium bromide when simultaneously bound to hamster mitotic cells.     

Effect of xenon on the excited States of phototropic receptor flavin in corn seedlings

The chemically inert, water-soluble heavy atom gas, xenon, at millimolar concentrations specifically quenches the triplet excited state of flavin in solution without quenching the flavin singlet excited state. The preferential quenching of the flavin triplet over the singlet excited state by Xe has been established by showing that the flavin triplet-sensitized photooxidation of NADH is inhibited while the fluorescence intensity and lifetime of flavin are not affected by Xe.     

Initial studies of a phytoestrogen-deoxyribonucleic acid interaction

Molecular modeling studies show that estrogens such as estradiol complement the topography of spaces between base pairs in unwound DNA and simultaneously hydrogen bond phosphate moieties on opposite strands. We demonstrate here that the phytoestrogen coumestrol has this capability, in addition to its documented properties of UV absorbance at lambda greater than 300 nm and fluorescence. The latter properties enable spectroscopic examination of interactions with DNA by methods not possible with estrogenic steroids. On exposure to calf thymus DNA, the UV spectrum of coumestrol displays a bathochromic shift and simultaneous hypochromic effect with an isosbestic point at 370 nm, suggesting a shift between coexisting free and bound states. Similar results are observed with the intercalating agents adriamycin, ethidium bromide, and acridine. The fluorescence spectrum of coumestrol is quenched on exposure to DNA as are those of adriamycin and acridine. Coumestrol differs from the intercalators in that denatured DNA does not affect its UV spectrum or alter its relative fluorescence yield. Unlike classical intercalators, coumestrol has no influence on the thermal stability of calf thymus DNA. Preliminary electrophoretic analysis of DNA plasmid conformers indicates that coumestrol is incapable of significantly altering DNA superhelical density, in contrast to ethidium bromide. These initial physicochemical data provide evidence for the DNA base-estrogen electronic and/or hydrophobic interactions suggested by modeling studies, yet tend to rule out classical intercalation as an explanation for these phenomena.