Complex formation of acridine orange with single-stranded polyriboadenylic acid and 5′-AMP: Cooperative binding and intercalation between bases

The binding of acridine orange to single-stranded polyribonucleic acid at low polymer to dye ratios exhibits cooperative behavior of the kind observed with other simple polyanions. It is thus attributed to electrostatic interaction between polymer and stacked dye molecules. At higher polymer to dye ratios, however, distinct deviations from the predictions of the basic theory occur. These are interpreted by additional non-cooperative binding of acridine orange to the bases of the polymer subunits owing to dye-base stacking. This effect is studied also with 5-AMP monomers where it likewise leads to complex formation. Both systems are investigated experimentally by means of the changes produced in the dye spectrum. Based on quantitative analyses the equilibrium constants of both systems are evaluated and discussed. They indicate a sandwich-type of intercalation of dye between two bases of the single-stranded polymer.     

Interaction between acridine orange and polyriboadenylic acid

The absorption spectra and circular dichroism of aqueous solutions of acridine orange mixed with polY(riboadenylic acid) [poly(rA)] have been measured for different mixing ratios at acid and neutral pH. The binding ratio of dye to poly(rA) has been determined by equilibrium dialysis. At acid pH where poly(rA) is in a double-stranded helix, monomeric dye molecules are intercalated between base pairs, first sparsely and then at neighbouring sites with mutual coupling, as the nucleotide-to-dye mixing ratio decreases. In the presence of excess dye, dimeric dye molecules of antiparallel type are bound to phosphate groups electrostatically and stack together to form linear sequences along a poly(rA) chain. At neutral pH where poly(rA) is single-stranded, isolated intercalation of monomeric dye molecules can occur in the helical parts. At intermediate mixing ratios, half-intercalated dimeric dye molecules are bound to adjacent sites and electronically coupled, inducing characteristic circular dichroism. In the presence of higher amounts of dye, external stacking of dimeric dye molecules of antiparallel type occurs along a poly(rA) chain. The binding of dye cations is suppressed to some degree at acid pH compared to that at neutral pH, owing to the repulsion exerted by protonated adenine bases.     

Differences in the red fluorescence of acridine orange bound to single-stranded RNA and DNA.

Fluorescence of acridine orange bound to RNA or DNA in the single-stranded form including single-stranded synthetic polyribo- or polydeoxyribonucleotides was measured in the expectation that some distinct structural characteristic between single-stranded RNA and DNA might be reflected by a specific fluorescent behaviour of bound dyes. It was found that the complex of the dye with single-stranded RNA emits a weaker red fluorescence around 650 nm than the complex with single-stranded DNA at low phosphate-to-dye ratios. The fact could be explained neither by a direct interaction of bound dyes with the 2′-hydroxyl group of ribose in RNA nor by the difference in the G-C content of the nucleic acids. On the basis of the character of dye molecules emitting the red fluorescence, it was suggested that the bases in single-stranded RNA might be buried in some hydrophobic environment that would make the dyes less likely to interact with them, compared with the bases in single-stranded DNA. It was further inferred that some conformational rigidity of single-stranded RNA may partially be responsible for the weaker red fluorescence.     

10N-nonyl acridine orange interacts with cardiolipin and allows the quantification of this phospholipid in isolated mitochondria.

The acridine orange derivative, 10N-nonyl acridine orange, is an appropriate marker of the inner mitochondrial membrane in whole cells. We use membrane model systems to demonstrate that 10N-nonyl acridine orange binds to negatively charged phospholipids (cardiolipin, phosphatidylinositol and phosphatidylserine). The stoichiometry has been found to be 2 mol 10N-nonyl acridine orange/mol cardiolipin and 1 mol dye/mol phosphatidylserine or phosphatidylinositol, while, with zwitterionic phospholipids, significant binding could not be detected. The affinity constants were 2 x 10(6) M-1 for cardiolipin-10N-nonyl-acridine-orange association and only 7 x 10(4) M-1 for that of phosphatidylserine and phosphatidylinositol association. The high affinity of the dye for cardiolipin may be explained by two essential interactions; firstly an electrostatic interaction between the quaternary ammonium of nonyl acridine orange and the ionized phosphate residues of cardiolipin and secondly, hydrophobic interactions between adjacent chromophores. A linear relationship was demonstrated between the cardiolipin content of model membranes and the incorporated dye. Consequently, a convenient and rapid method for cardiolipin quantification in membranes was established and applied to the cardiolipin-containing organelle, the mitochondrion.     

Induced optical activity of acridine orange bound to poly-S-carboxymethyl-L-cysteine

The absorption and rotatory properties of acridine orange-poly-S-carboxymethyl-L -cysteine system in water and in 0.2 M NaCl have been measured at different pH and polymer-to-dye mixing ratios. The absorption spectra indicate that the dyes are bound to the polymer in dimeric or highly aggregated forms. At neutral pH where the polymer is randomly coiled, no optical activity is induced on the absorption bands of bound acridine orange. At acid pH where the polymer has the β-conformation, a pair of positive and negative circular dichroic bands occur at each of the absorption bands, centered around 458 and 261 mμ. The signs of those bands are opposite to those found for α-helical poly-L -glutamic acid. A model for the binding of dye to the β-form polymer is presented, in which dimeric dyes are attached to ionized carboxyl groups and slack one another to form linear arrays on both sides of an extended polypeptide chain. The observed circular dichroism spectra can be explained by the Tinoco's exciton mechanism, based on this model. Low molecular weight poly-S-carboxymethyl-L -cysteine induces quite a different circular dichroism on bound acridine orange.     

Absorption and fluorescence studies on interaction between cationic dyes and Klebsiella K7 capsular polysaccharide.

Interaction of cationic dyes, pinacyanol chloride, acridine orange and phenosafranin, with Klebsiella K7 capsular polysaccharide has been investigated by spectrophotometric and spectrofluorometric measurements. The acidic polysaccharide induce a metachromatic blue shift of the absorption band of pinacyanol chloride from 600 nm to 495 nm, indicating strong metachromasy. Stoichiometry of polyanion and dye cation (1:1.5) in the polymer-dye compound formed by the interaction between pinacyanol chloride dye and K7 polymer indicate that both glucuronic acid and pyruvic acid act as the potential anionic sites for interaction. Both spectrophotometric titration of pinacyanol chloride and spectrofluorometric titration of acridine orange and phenosafranin dyes by the polymer gave quite comparable equivalent weights for the polymer. Dye-polymer interaction studies indicated induction of metachromasy in the cationic dye by the anionic biopolymer, establishing its chromotropic character.     

Competitive interaction of serotonin and the dye acridine orange with DNA

The interaction of serotonin and acridine orange dye with DNA isolated from bacterium Escherichia coli and the yeast Candida utilis has been analysed by spectrofluorimetric method. Using data on competitive binding to DNA of serotonin and acridine orange, known as DNA intercalator, a conclusion concerning the formation of intercalated complex between serotonin and DNA has been made. It is shown that for yeast DNA the constant of intercalated binding of serotonin is 3,5-fold smaller than for the bacterial one.     

Structure and optical activity of the DNA-aminoacridine complex

The electronic absorption and circular dichroism spectra of the DNA-acridine orange complex have been measured over a range of ionic strength, pH, and DNA phosphate to dye (P/D) ratios. Three circular dichroism bands associated with the long wavelength absorption band of acridine orange are induced on complex formation with DNA. Two of the dichroism bands, due mainly to dimeric dye molecules, are favored by low ionic strength, low pH (3.2), and a low P/D ratio (～3), while the third, deriving primarily from monomeric dye, is optimum at high ionic strength, neutral pH, and a larger P/D ratio (9). The data suggest that monomeric acridine orange binds to DNA in the form of a left-handed helical array with four dye molecules per turn, while the bound dimer has a skewed sandwich conformation which is itself dissymmetric. The stereochemical relations between the bound monomer dye and the DNA are consistent with a modified intercalation model for the DNA-acridine complex.     

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.     

Red cell phosphoglycerate mutase and bisphosphoglycerate synthase: controlled modifications in coulombic properties in vitro.

Fluorimetric titrations of acridine orange and heparin indicate that the equivalent weight of the latter can be related to its anticoagulant activity. Pulse radiolysis has been used to compare the binding of acridine orange and poly-L-lysine with several heparins of differing biological activities. Although correlation with biological activity can be made, the dye and poly-L-lysine differ in their binding characteristics to heparin.     

Quantitative evaluation of the uptake capacity of intact thrombocytes using fluorescent dyes

A new approach to quantitative determination of fluorescent dye uptake by intact cells is suggested. Fluorescent amine acridine orange selectively accumulating in 5HT granules of platelets has been used. Fluorescence signal analysis allows the estimation of a relative granule volume and the ratios of acridine orange transfer over cytoplasmic and granule membranes. The following results were obtained in human and rabbit platelets: a relative granule size was 14 +/- 1 % and 29 +/- 2 % of the total cell volume, intra-granule to extra-granule dye concentration ratios were 2260 +/- 382 and 30000 +/- 5550, while intra-cytoplasm to extra-cytoplasm concentration ratios were 375 +/- 60 and 225 +/- 60, respectively.     

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.     

Interactions of nucleic acids with fluorescent dyes: spectral properties of condensed complexes.

Interaction of cations with nucleic acids (NA) often results in condensation of the product. The driving force of aromatic cation-induced condensation is the cooperative interaction between ligand and single-stranded (ss) NA. This type of reaction is highly specific with regard to the primary and secondary structure of NA, and results in destabilization of the latter. The spectral properties of fluorescent intercalating and non-intercalating ligands [acridine orange, pyronin Y(G), DAPI, Hoechst 33258, and Hoechst 33342]-NA complexes were studied in both the relaxed and condensed form. The changes in absorption, excitation, and fluorescence emission spectra and fluorescence yield that followed the condensation were examined. Although some of these effects can be explained by changes in solvation of the fluorophore and its interaction with NA bases and the solvent, the overall effect of condensation on spectral properties of the complex is unpredictable. In particular, no correlation was found between these effects and the ds DNA binding mode of these ligands. Nevertheless, the spectral data associated with polymer condensation can yield information about the composition and structure of NA and can explain some nonspecific interactions of these probes.     

Thermodynamics of mucopolysaccharide–dye binding. I. Identification of free and bound dye via membrane filtration: Acridine orange–dermatan sulfate system

Stoichiometric mixtures of acridine orange with dermatan sulfate at total dye concentrations ? 1 × 10^?5 M show fluorescence maxima at 540 nm and 660 nm on excitation at 436 nm. By means of membrane filtration, it is directly demonstrated that the species emitting at 540 nm is due only to unbound dye whereas the 660-nm emitting species is due to bound dye. It is, therefore, possible to differentiate unbound acridine orange from its dermatan sulfate complex solely by spectroscopic methods. Thermodynamic binding parameters can be calculated from rapid spectroscopic measurements without disturbing the system.     

Thermodynamics of mucopolysaccharide–dye binding. III. Thermodynamic and cooperativity parameters of acridine orange–heparin system

Binding isotherms for acridine orange (AO)–heparin systems can be evaluated solely on the basis of quantitative fluorescence spectroscopic measurements. The evaluation of thermodynamic parameters indicates that the interactions of AO with heparins from several animal sources are similar to each other in magnitude. Binding is highly exothermic (ΔH = ?6 kcal mol^?1) and is stabilized by dye–polymer and dye–dye (coopertive) interactions, as well as by entropic factors (ΔS = +7 e.u.). The predominant stabilizing factor appears to be the electrostatic attraction between the AO cation and the heparin polyanion, although the other factors are important as well. At 24°C the value of the cooperative binding constants for the various heparins range from 8.8 to 11.3 × 10⁵M^?1, corresponding to a free energy of ?8 kcal mol^?1. The degree of cooperativity, which is a direct measure of dye–dye interaction, varies with polymer:dye ratio; the theoretical basis for this variation remains to be elucidated. Electrophoretic data indicate that each heparin sample consists of a mixture of species, each with its own charge density. This precludes definitive interpretation of observed small differences in the values of the thermodynamic parameters among the various samples until each sample can be resolved into its components.     

Absorption and Fluorescence Spectra of Euchrysine Ggnx and Acridine Orange; Effects of Heparin, NaCl and a Cation Exchange Resin

The absorption and fluorescence spectra of two samples of dye labeled euchrysine were found to differ. One sample, labeled GGNX, had absorption and fluorescence maxima of 435 and 515 nanometers (nm) respectively. The other sample was not further labeled, but had absorption and fluorescence maxima of 492 and 535 nm. The latter values, as well as the shape of both the fluorescence and absorption curves of the second sample were superimposable on a recrystallized sample of acridine orange labeled correctly C. I. 46905. Euchrysine has two free amino groups which are fully methylated in acridine orange, therefore a nitrous acid test can differentiate the two dyes. The sample of euchrysine labeled GGNX gave a reaction, as did acridine yellow, C. I. 46025, but acridine orange, C. I. 46005, did not. Fluorescence metachromasy of euchrysine is less efficient than that of acridine orange in two ways: the shift in the spectrum is smaller by about 40 nm, making the separation of the colors more difficult both visually and by instruments and the metachromatic fluorescence has less than half of the intensity of acridine orange as measured at the peak for each dye. Confusion between these two dyes has occurred because suppliers have used the names interchangeably. For critical studies, the dye used should be identified by its Colour Index number.     

Induced Cotton effects of tRNA-acridine orange complex and tRNA conformation

Circular dichroism spectra of acridine orange bound to E. coli tRNA were studied at varying tRNA phosphate-to-dye (P/D) ratios for both unfractionated and purified materials in the absence of Mg⁺⁺. From the rather discrete features exhibited in the circular dichroism spectra three types of interactions were observed: (1) A high P/D ratio such as 75.2 or 49.8 indicates the interaction between the nucleotide base and dye molecule. The spectra with a large positive peak at 515 mμ are, however, quite different from that of DNA–AO complex under similar conditions. (2) With an intermediate P/D ratio (26.5 to 9.6) dye molecules bound strongly to the polynucleotide chain. (3) With low P/D ratios (≤7.5) the interaction appears to be due to the stacked dye molecules in the single-stranded part of tRNA. The spectra of the third group have an isobestic point at 477 mμ. Below a P/D ratio of 4 the spectrum shows one positive and two negative bands which may be the characteristics of circular dichroism of stacked dyes in polynucleotide chain. Although no drastic change in the conformation of tRNA itself was detectable in the presence of Mg⁺⁺ in the ultraviolet region, a dramatic change was observed in the circular dichroism of tRNA–acridine orange complex when Mg⁺⁺ concentration was increased to 10^?3M. It was inferred that certain conformational changes other than simple hydrogen bond formation occured in tRNA molecules at this high Mg⁺⁺ concentration, so that the amount of bound dye in the stacking condition was increased through the transition.     

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.     

Kinetic studies of interaction between acridine orange and DNA

The interaction between acridine orange (AO) and deoxyribonucleic acid (DNA) was studied by the stopped-flow method. The spectral change of AO due to interaction with DNA was followed over the wavelength range 350–600 nm at various concentration ratios of DNA phosphate to dye. The spectral change observed by the stopped-flow method was found distinctly different from that, during the dead-time, leading to a conclusion that the binding of AO to the outside of DNA occurs much faster than the intercalation into base pairs of DNA. The dependence of the rate of reaction on the reactant concentration and on the salt, concentration of the solution was also studied. The results are consistent with the mechanism that the intercalation proceeds via the outside bound state.     

Optimization of flow-cytometric discrimination between reticulocytes and erythrocytes

An automatized technique to count reticulocytes by means of flow cytometry is described. Blood samples were stained by the fluorescent dye acridine orange without the use of fixative. Scatter and red fluorescence of the blood cells were measured in a flow cytometer. A discrimination between reticulocytes and erythrocytes was only achieved by using logarithmic amplification. The discrimination was better in peak mode than in area mode. The optimum dye concentration was 0.5 mg/liter acridine orange. At lower dye concentrations, not all reticulocytes were measured, whereas at higher dye concentrations the degree of discrimination between reticulocytes and erythrocytes decreased. There was a suitable discrimination between reticulocytes and erythrocytes. The reticulocyte numbers were scored by flow cytometry as well as by microscope for blood samples with 0.1-14% reticulocytes. The correlation between both methods was close.