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Polyelectrolyte complex (polyplex) formation was studied by employing tapping mode atomic force microscopy (AFM) and an ethidium bromide fluorescence assay. The polycations chitosan and poly-L-lysine were used to compact DNA and the stability of the polyplexes was evaluated upon exposure to competing polyanions (alginate and xanthan). Furthermore, the relative preference of these polycations for DNA and the competing polyanion was investigated. The results showed that neither poly-L-lysine nor chitosan displayed any selectivity in binding to DNA relative to the competing polyanions, demonstrating the importance of electrostatics in the binding of a polycation to a polyanion. However, the ability of the polyanions to destabilize the DNA-polycation complexes depended on both the polyanion and the polycation employed, indicating that polymer-specific properties are also important for the complexation behavior and polyplex stability. Destabilization experiments further showed that annealing yielded complexes that were less prone to disruption upon subsequent exposure to alginate. Annealing experiments of plasmid DNA-chitosan complexes showed an increased fraction of rods following temperature treatment, indicating that the rods most likely are the more stable morphology for this system.

RNA plays a pivotal role in the replication of all organisms, including viral and bacterial pathogens. The development of small molecules that selectively interfere with undesired RNA activity is a promising new direction for drug design. Currently, there are no anti-HIV treatments that target nucleic acids. This article presents the HIV-1 Rev response element (RRE) as an important focus for the development of antiviral agents that target RNA. The Rev binding site on the RRE is highly conserved, even between different groups of HIV-1 isolates. Compounds that inhibit HIV replication by binding to the RRE and displacing Rev are therefore expected to retain activity across groups of genetically diverse HIV infections. Systematic evaluations of both the RRE affinity and specificity of numerous small molecule inhibitors are essential for deciphering the parameters that govern effective RRE recognition. This article discusses fluorescence-based techniques that are useful for probing a small molecule's RRE affinity and its ability to inhibit Rev-RRE binding. Rev displacement experiments can be conducted by observing the fluorescence anisotropy of a fluorescein-labeled Rev peptide, or by quantifying its displacement from a solid-phase immobilized RRE. Experiments conducted in the presence of competing nucleic acids are useful for evaluating the RRE specificity of Rev-RRE inhibitors. The discovery and characterization of new RRE ligands are described. Eilatin is a polycyclic aromatic heterocycle that has at least one binding site on the RRE (apparent Kd is approximately 0.13 microM), but it does not displace Rev upon binding the RRE (IC50 > 3 microM). In contrast, ethidium bromide and two eilatin-containing metal complexes show better consistency between their RRE affinity and their ability to displace a fluorescent Rev peptide from the RRE. These results highlight the importance of conducting orthogonal binding assays that establish both the RNA affinity of a small molecule and its ability to inhibit the function of the RNA target. Some Rev-RRE inhibitors, including ethidium bromide, Lambda-[Ru(bpy)(2)eilatin]2+, and Delta-[Ru(bpy)(2)eilatin]2+ also inhibit HIV-1 gene expression in cell cultures (IC50 = 0.2-3 microM). These (and similar) results should facilitate the future discovery and implementation of anti-HIV drugs that are targeted to viral RNA sites. In addition, a deeper general understanding of RNA-small molecule recognition will assist in the effective targeting of other therapeutically important RNA sites.

The permeability of bacteriophage T4 and the change in T4 permeability caused by mutation to osmotic shock resistance are investigated here by quantification of the kinetics with which both a DNA-specific probe (ethidium) and a protein-specific probe [1,1'-bi(4-anilino)naphthalene-5,5'-di-sulfonic acid, or bis-ANS)] bind to T4. In the case of an osmotic shock-resistant mutant, T40s41, both ethidium and bis-ANS bind with first order kinetics. The first-order rate constant (k*) for both bis-ANS and ethidium is a function of anion type and concentration. Adenosine triphosphate, phosphate, bisulfite, sulfate, and acetate anions all reduce k* below the k* observed when chloride is the only anion. When chloride is the only anion at 25 degrees C, k* values for binding to T40s41 are orders of magnitude above k* values for binding to wild-type T4 (T4wt). At 25 degrees C, k* for T4wt is too small to measure but k* for T4wt increases at 50-55 degrees C to values approaching those measured for T40s41, without inactivating T4wt, when chloride is the only anion; during heating, T4wt is stabilized by both ethidium and bis-ANS. Binding to T4wt is reversible at 50-55 degrees C, but not at 25 degrees C. Equilibrium binding of bis-ANS to T40s41 reveals 112 +/- 24 sites per T4 capsid. Equilibrium binding of ethidium to T40s41 reveals both high- and low-affinity sites previously observed in the packaged DNA of other bacteriophages. The ATP-induced decrease in k* is not accompanied by a decrease in equilibrium binding. The following hypotheses are presented to explain the above data: (a) All detected bis-ANS binding sites on T4 are interior to the outer surface of T4. (b) The value of k* for both bis-ANS and ethidium is controlled at the port(s) of passage through the outer shell of the T4 capsid. (c) The anions present control k* values at the port(s) of entry, probably by controlling the size of this port. The effects on k* of phosphate explain the otherwise paradoxical observation [P. J. McCall and V. A. Bloomfield (1976) Biopolymers 15, 2323-2336] that in a phosphate buffer the permeabilities of T4wt and T40s41 are the same.

A flow linear dichroism technique is utilized to study the unwinding of supercoiled DNA induced by the binding of ethidium bromide (EB) and proflavine (PF) at different ratios r (drug added/DNA base). In the case of either EB or PF bound to linear calf thymus DNA, the reduced linear dichroism signals LD/A (LD: linear dichroism; A: absorbance, both measured at the same wavelength), determined at 258, and 520 or 462 nm (corresponding to contributions predominantly from the partially oriented DNA bases, intercalated EB, or PF, respectively) are nearly independent of drug concentration. In the case of supercoiled DNA, the magnitude of LD/A at 258 nm first increases to a maximum value near r = 0.04–0.05, and then decreases as r is increased further, mimicking the behavior of the sedimentation coefficients, viscosities, and gel electroporphoresis patterns measured by other workers at similar values of r. However, LD/A at 520 nm, which is due to DNA-bound EB molecules, is constant within the range of r values of 0.02–0.06 in which the magnitude of LD/A determined at 258 nm due to the DNA bases exhibits a pronounced maximum. In contrast, in the case of PF, the magnitudes of LD/A determined at 258 or 462 nm are characterized by similar dependencies on r, both exhibiting pronounced maxima at r = 0.05; this parallel behavior is expected according to a simple interacalation model in which the DNA bases and drug molecules are stacked on top of one another, and in which both are oriented to similar extents in the flow gradient. The unexpected differences in the dependencies of (LD/A)258 and (LD/A)520 on r in the case of EB bound to supercoiled DNA, are attributed to differences in the net overall alignment of the EB molecules and DNA bases in the flow gradient. The magnitude of the LD signal at 258 nm reflects the overall degree of orientation of the supercoiled DNA molecules that, in turn, depends on their hydrodynamic shapes and sizes; the LD signals characterizing the bound EB molecules may reflect this orientation also, as well as the partial alignment of individual DNA segments containing bound EB molecules. The differences in the LD characteristics of the bound PF and EB molecules may be due to subtle differences in the mechanisms of binding, perhaps reflecting differences in the torsional dynamics and local rigidities in superhelical DNA [Wu et al. (1988) Biochemistry27, 8128–8144] induced by these two different in tercalating agents.

Calorimetric titrations have been performed on the binding of ethidium and propidium to calf thymus DNA at temperatures in the 15-60 degrees C range. Enthalpy changes (delta HB) derived from these experiments performed with the new Omega reaction calorimeter have a precision of +/- 0.10 kcal/mol or less at all temperatures. For ethidium (a monocation), delta HB varies little with temperature, and the heat capacity change (delta CP) for the binding reaction derived from these parameters is 10 cal/deg/mol. In contrast, delta HB changes from -6.5 to -8.1 kcal/mol for DNA binding of propidium (a dication due to a charged amine group at the end of an alkyl chain attached to the phenanthridine ring nitrogen), and delta CP is -57 cal/deg/mol. At 21 degrees C a plot of delta HB vs mole ratio is curved downward for propidium in the 0.08-0.25 range, whereas the same plot at 45 degrees C is a straight line from 0.05 to 0.15 and sharply downward thereafter. Similar plots for ethidium follow the latter pattern between 25 and 50 degrees C. These observations and our analyses of delta HB and delta SB are consistent with the hypothesis that the location in the DNA complex and the rotational motion of the alkylamine chain change substantially over the temperature range in this study. Only near 50 degrees C is delta HB equal for the binding of these two cations to DNA, and caution must be used in analyses of enthalpic effects when the temperature dependence for delta HB is not available.

Upon increasing the concentration of ethylene glycol (EG) at 37°C, the twist energy parameter, ET, which governs the supercoiling free energy, was recently found to undergo a decreasing (or reverse) sigmoidal transition with a midpoint near 20 w/v % EG. In this study, the effects of adding 20 w/v % EG on the torsion elastic constant (α) of linear p30δ DNA and on the hydrodynamic radius (RH) of a synthetic 24 bp duplex DNA were examined at both 40 and 20°C. The time-resolved fluorescence intensity and fluorescence polarization anisotropy (FPA) of intercalated ethidium were measured in order to assess the effects of 20 w/v % EG on: (1) α; (2) RH; (3) the lifetimes of intercalated and non-intercalated dye; (4) the amplitude of dye wobble in its binding site; and (5) the binding constant for intercalation. The effects of 20 w/v % EG on the circular dichroism (CD) spectrum of the DNA and on the emission spectrum of the free dye were also measured. At 40°C, addition of 20 w/v % EG caused a substantial (1.27- to 1.35-fold) increase in α, a significant change in the CD spectrum, and a very small, marginally significant increase in RH, but little or no change in the amplitude of dye wobble in its binding site or the lifetime of intercalated dye. Together with previously reported measurements of ET, these results imply that the bending elastic constant of DNA is significantly decreased by 20 w/v % EG at 40°C. At 20°C, addition of 20 w/v % EG caused a marginally significant decrease in α and very little change in any other measured properties. Also at 20°C, addition of 30 w/v % betaine caused a marginally significant increase in α and significant but modest change in the CD spectrum, but very little change in any other properties. © 2006 Wiley Periodicals, Inc. Biopolymers 85: 222–232, 2007. This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com

The influence of mica surface on DNA/ethidium bromide interactions is investigated by atomic force microscopy (AFM). We describe the diffusion mechanism of a DNA molecule on a mica surface by using a simple analytical model. It appears that the DNA diffusion on a mica surface is limited by the surface friction due to the counterion correlations between the divalent counterions condensed on both mica and DNA surfaces. We also study the structural changes of linear DNA adsorbed on mica upon ethidium bromide binding by AFM. It turns out that linear DNA molecules adsorbed on a mica surface are unable to relieve the topological constraint upon ethidium bromide binding. In particular, strongly adsorbed molecules tend to be highly entangled, while loosely bound DNA molecules appear more extended with very few crossovers. Adsorbed DNA molecules cannot move freely on the surface because of the surface friction. Therefore, the topological constraint increases due to the ethidium bromide binding. Moreover, we show that ethidium bromide has a lower affinity for strongly bound molecules due to the topological constraint induced by the surface friction.

The factors that determine the binding of a chromophore between the base pairs in DNA intercalation complexes are dissected. The electrostatic potential in the intercalation plane is calculated using an accurate ab initio based distributed multipole electrostatic model for a range of intercalation sites, involving different sequences of base pairs and relative twist angles. There will be a significant electrostatic contribution to the binding energy for chromophores with a predominantly positive electrostatic potential, but this varies significantly with sequence, and somewhat with twist angle. The usefulness of these potential maps for understanding the binding of intercalators is explored by calculating the electrostatic binding energy for 9-aminoacridine, ethidium, and daunomycin in a variety of model binding sites. The electrostatic forces play a major role in the positioning of an intercalating 9-aminoacridine and a significant stabilizing role in the binding of ethidium in its sterically constrained position, but the intercalation of daunomycin is determined by the side-chain binding. Sequence preferences are likely to be determined by a complex and subtle mixture of effects, with electrostatics being just one component. The electrostatic binding energy is also unlikely to be a major determinant of the twist angle, as its variation with angle is modest for most intercalation sites. Overall, the electrostatic potential maps give guidance on how positively charged chromophores can be chemically adapted by heteroatomic substitution to optimise their binding.

The thermodynamical parameters (free energy, enthalpy, and entropy) of complex formation between ethidium bromide and single-stranded and double-stranded tetranucleotides of different base sequence [5-d(TpGpCpA), 5-d(ApCpGpT), and 5-d(ApGpCpT) have been determined from the temperature dependencies of 500 MHz proton nmr chemical shifts. The analysis enables the contributions to be differentiated for the formation of different types of complexes (1:1, 2:1, 1.2 and 2:2) in aqueous solution. The results have been interpreted in terms of the main types of intermolecular interactions responsible for formation of the different complexes; van der Waals and electrostatic interactions are important for formation of complexes of ethidium bromide with single-stranded tetranucleotides, whereas van der Waals and hydrophobic interactions play a significant role in the binding of the dye to the tetramer duplexes.

Complexation of the trypanocidal drug, ethidium bromide (EB), and the self-complementary deoxytetraribonucleoside triphosphates, 5'-d(ApCpGpT), 5'-d(ApGpCpT), and 5'-d(TpGpCpA), in aqueous salt solution has been investigated using one-dimensional and two-dimensional 500/600 MHz 1H-nmr spectroscopy. Six hundred megahertz two-dimensional homonuclear 1H-nmr spectroscopy (nuclear Overhauser effect spectroscopy) was used for a qualitative determination of the structures of EB binding with the deoxytetranucleotides. Concentration dependencies of proton chemical shifts of the molecules have been measured at constant temperatures (T = 303 or 308 K). Different successive schemes of complex formation between the dye molecule and the tetranucleotides have been examined by taking into account various molecular associations in solution, viz., 1:1, 1:2, 2:1 and 2:2 complexes. Equilibrium reaction constants and the limiting proton chemical shifts in the complexes have been determined. The relative contributions of different types of complexes in the equilibrium mixture have been determined and special features of the dynamic equilibrium have been revealed by analysis of chemical shifts as a function of both the dye and tetranucleotide concentrations. The present analysis leads to the conclusion that EB binds preferentially to the pyrimidine-purine sites of the tetranculeotide duplexes. The results show that the energy of EB binding depends on the base content in the pyrimidine-purine sites of the tetramers and on the nucleotide residuals flanking the preferential site. The most favorable structures of the 1:2 and 2:2 complexes of the dye with the tetranucleotides have been constructed using calculated values of induced chemical shifts of EB protons in conjunction with intermolecular nuclear Overhauser effects. The structures of the EB: tetranucleotide complexes depend on tetramer base sequence and are characterized by differences in helix parameters.

Fluorescence resonance energy transfer among linear DNA bound fluorophores was carried out to study the process in one dimension. The donor fluorescence intensity decays in the case of energy transfer in one dimension are stretched exponential and show exp[-(t/τ)1/6] time dependence, which results in an initial more rapid decay and subsequent slower decay at long times when compared to those in higher dimensions. DNA-bound 4′,6′-diamidino-2-phenyl indole (DAPI), acridine orange (AO), and ethidium bromide (EB) were used as donors. The acceptors were in the case of DAPI AO and EB; in the case of AO nile blue (NB), methylene blue (MB), and crystal violet (CV); and NB, MB, and oxazine 750 in the case of EB. As expected, the donor intensity decays became highly heterogeneous upon energy transfer and were characterized by the simultaneous presence of both highly and marginally quenched donors. The intensity decays for all three donors in the presence of various acceptors are satisfactorily described by the Forster model of energy transfer in one dimension. The intensity decays also allow for clear rejection of a two- or three-dimensional model. The experimentally recovered critical Forster distances (R0) ranged between 37 A in the case of DAPI and EB to 70 A in the case of AO and CV donor-acceptor pairs. These recovered R0 values compare reasonably with those calculated from spectral properties if we use values of 1.25 for κ2, and 1.5 for the refractive index of DNA. The κ2 value will be even higher, between 1.5 and 2.0, if the consensus DNA refractive index of 1.75 is used. These κ2 values strongly suggest that the dipoles of the acceptor chromophores when bound to DNA are not randomly oriented but are aligned preferentially in plane. © 1995 John Wiley & Sons, Inc.

DNA molecules ranging in size from 1 to 630 kilobase pair and intercalated with either ethidium bromide (EtBr) or propidium iodide (PI) were electrophoresed in 1% agarose at four different electric field strengths. The extent of intercalation of EtBr under the conditions of our electrophoresis experiments was determined by a spectroscopic technique, whereas the extent of intercalation of PI was inferred from previous studies. The effects of the increase in DNA contour length and the concomitant decrease of linear charge density were separated based on our analysis of the mobility data. We conclude that the main factor responsible for the reduced electrophoretic mobility of intercalated DNA is the diminished linear charge density and not the increased contour length. © 1994 John Wiley & Sons, Inc.

A rigorous theory is developed for ethidium binding to linear and circular DNAs and for the ratios of topoisomers produced upon ligation of an equilibrium population of noncovalently closed circles in the presence of ethidium. Assuming an unwinding angle ϕE = 26° for intercalated ethidium, optimum values of the intrinsic binding constant, KE = 7.16 × 104M−1, the intrinsic twist, l0 = 23.746 turns, and twist energy parameter, Et = 5250, are obtained by fitting the present theory to the data of Shore and Baldwin [(1993) Journal of Molecular Biology, Vol. 170, pp. 983–1007] for a 247 base pair DNA. A very good fit is achieved with these optimum values, but a poor fit results when the parameters estimated by Shore and Baldwin are employed in the same theory. Three assumptions employed in the analysis of Shore and Baldwin are found to be not strictly valid. Adoption of the present substantially larger Et value as representative of their short DNAs would allow the Et vs N data of Shore and Baldwin to conform to the shape predicted by Shimada Yamakawa [(1985) Journal of Molecular Biology, Vol. 184, pp. 319–329] and Frank-Kamenetskii et al. [(1985) Journal of Biomolecular Structure and Dynamics, Vol. 2, pp. 1005–1012], and would imply that all of their DNAs exist in a substantially stiffer than normal state. © 1994 John Wiley & Sons, Inc.

Individual ethidium-stained DNA molecules, embedded in an agarose gel made with electrophoresis buffer (0.05 molar salt), are observed using a fluorescence microscope. In the first experiment, open circular 66 kilobase pair (kbp) plasmids, immobilized by agarose fibers threaded through their centers, display entropic "rubber" elasticity. The charged molecules extend in an electric field of several volts per centimeter and contract to a compact random coil when the field is removed. The extension of the plasmids as a function of field strength is consistent with the freely jointed chain model when the effective electrophoretic charge density is set at 15 e-per persistence length. In a second experiment, stained linear 48.5 kbp DNA molecules are observed as random coils immobilized in agarose. A measure of their size, here named the "maximal-X-extent," is taken for 100 molecules and found to average 1.47 mu. A Monte Carlo computer simulation of random coils (freely jointed chain model) gives the same maximal-X-extent value when the persistence length is set at 0.08 mu.

The solution complexes of ethidium bromide with nine different deoxydinucleotides and the four self-complementary ribodinucleoside monophosphates as well as mixtures of complementary and noncomplementary deoxydinucleotides were studied as models for the binding of the drug to DNA and RNA. Ethidium bromide forms the strongest complexes with pdC-dG and CpG and shows a definite preference for interaction with pyrimidine–purine sequence isomers. Cooperativity is observed in the binding curves of the self-complementary deoxydinucleotides pdC-dG and pdG-dC as well as the ribodinucleoside monophosphates CpG and GpC, indicating the formation of a minihelix around ethidium bromide. The role of complementarity of the nucleotide bases was evident in the visible and circular dichroism spectra of mixtures of complementary and noncomplementary dinucleotides. Nuclear magnetic resonance measurements on an ethidium bromide complex with CpG provided evidence for the intercalation model for the binding of ethidium bromide to double-stranded nucleic acids. The results also suggest that ethidium bromide may bind to various sequences on DNA and RNA with significantly different binding constants.

Equilibrium binding of ethidium, quantitated by fluorescence enhancement, to DNA packaged in bacteriophage T7 and T7 deletion mutants has been compared with the binding of this dye to DNA released from its capsid (free DNA). During achievement of apparent equilibrium binding, no change in bacteriophage T7 structure occurred, by the criterion of agarose gel electrophoresis. However, excessive incubation with ethidium bromide caused detectable changes in bacteriophage structure, a possible explanation of disagreements in similar studies previously performed with T-even bacteriophages. Scatchard plots for packaged DNA had a curvature greater than the previously demonstrated [Bresloff, J. L. & Crothers, D. M. (1981) Biochemistry20, 3547–3553] curvature for free DNA. By treating plots for packaged DNA as though they were biphasic, it was found that binding to most sites occurred with an apparent association constant (Kap) 3.3–4.3 times lower than the Kap of free DNA. The number of these sites increased significantly as the density of packaged DNA was decreased by use of the deletion mutants. Values of ΔH° for these sites were negative and equal to the ΔH° for free DNA; values of ΔS° were positive and about half the ΔS° for free DNA. A second class of sites, roughly 1.2% of the total, had a significantly higher Kap and more negative ΔH° than those of the majority of sites.

Enthalpy changes (ΔHB) for the binding of ethidium (a monocation) and propidium (a dication) to calf thymus DNA have been determined calorimetrically in piperazine-N, N′-bis(2-ethanesulfonic acid) buffer with the fluoride ion as the counterion. Heats of dilution for the fluoride salts of ethidium and propidium were substantially less than the corresponding values found for other halide salts of these cations. At a Na+ ion concentrations of 0.019, ΔHB = −8.3 and −7.9 ± 0.3 kcal mol−1 for ethidium and propidium, respectively. For these two cations, just as was observed for the naphthalene monoimide (monocation) and diimide (dication) [H. P. Hopkins, K. A. Stevenson, and W. D. Wilson, (1986) J. Sol. Chem.15, 563–579], ΔHB is within the same experimental error for both cations. Apparently, charge–charge interactions in DNA–cation complexes produce only small changes in the enthalpy for the system. In the concentration range 0.019–0.207, the ΔHB values for propidium did not depend appreciably on the Na+ ion concentration, and a similar pattern was shown to exist for ethidium. When these results were combined with ΔGB values for the binding of these cations to DNA, we found the variation of ΔSB with Na+ ion concentration to be remarkably close to the predictions of modern polyelectrolyte theory, i.e., propidium binding to DNA causes approximately twice as many Na+ ions to be released into the bulk solution as does the binding of ethidium. The much stronger binding of propidium, relative to ethidium, at low ionic strengths is thus seen to be primarily due to entropic effects.

The effects of sodium ion concentration on the binding isotherms and association and dissociation reaction rates for the interaction of the closely related intercalating dication, propidium, and the monocation, ethidium, with DNA have been determined by spectrophotometric binding and stopped-flow kinetics methods. The binding of propidium to DNA is best described by a neighbor-exclusion binding isotherm (two base pairs per binding site) with negative ligand cooperatively on binding. The cooperativity parameter is fairly independent of salt concentration, while the log of the observed equilibrium binding constant varies with −log [Na+], with a slope of two for the propidium–DNA interaction. These effects of the sodium ion on the equilibrium binding of propidium with DNA are similar to those previously described for the dication, quinacrine [Wilson, W.D. & Lopp, I.G. (1979) Biopolymers, 18, 3025–3041]. Ethidium behaves, as a function of salt, as a monocation binding to DNA with neighbor exclusion and without ligand cooperativity. Equations are derived for two limiting kinetics models for intercalation involving binding of the intercalator to a preequilibrium, open state of DNA (model I) or binding form a preequilibrium externally associated state of the intercalator with DNA (model II). Model II gives the best fit to all of the kinetic results if it is assumed that the initial external interaction of the intercalator with DNA is similar to the exchange of free and condensed simple counterions. Intercalation then occurs from this state following an opening transition of the base pairs of the double helix. This model predicts a larger effect of salt concentration on the association than on the dissociation reaction, and that is what is experimentally observed. The intercalation conformational change makes a significant contribution to the ionic effects for both the equilibrium binding and the kinetic constants. The dissociation results and the association reaction results under pseudo-first-order conditions could be fit with single exponential curves under the conditions of our experiments.

The DNA–ligand interactions of a series of phenanthridinium compounds with various combinations of amino, azido, and hydrogen functions at R3 and R8 were examined to determine the contribution of these particular substituents to ligand binding. Spectrophometric titrations using calf-thymus DNA emphasized the importance of amino substituents in conferring a strong interaction and also stabilizing the interaction against reversal by high ionic strength. Although azido groups were not as effective as amino groups, they were more effective than hydrogen functions in enhancing the interaction. Furthermore, an amino substitution at R8 was consistently, though only slightly, more effective than an amino substituent at R3. The results from superhelical titrations using plasmid pBR322 DNA demonstrated that analogs with amino and/or azido functions at both R3 and R8 produced the greatest unwinding, and compounds with an amino or an azido function at R8 proved more effective than those with the corresponding amino or azido substituent at R3.

The enthalpies of binding of chloroquine and quinacrine to DNA at different molar ratios of drug to DNA and at different ionic strengths have been measured. The limiting values obtained with quinacrine fall in the range found for typical intercalating agents (e.g., ethidium, proflavin, adriamycin), whereas the value obtained with chloroquine is always zero, independent of the ratio of drug to DNA and ionic strength. The dilatometric measurements performed on the same systems and on the ethidium–DNA system show that when ethidium and quinacrine bind to DNA at low drug/DNA ratios, a volume decrease of about 16 mL/mol of bound drug occurs. No change in volume is observed when the two drugs bind to DNA through external, electrostatic forces. The volume change can be attributed to the loss of structured water around hydrophobic moieties of the drug molecules, following intercalation. In contrast, chloroquine binding to DNA at low drug/DNA ratios is characterized by a volume change distinctly smaller than that shown by quinacrine. The low ΔVB and ΔHB values shown by chloroquine are discussed in terms of the mechanism of interaction with DNA.

Circular dichroism spectroscopy has been used to investigate the influence of DNA molecular size, base composition, and the presence of intercalating agents upon the Ψ transition of DNA brought about by high concentrations of poly(ethylene oxide) and salt (Lerman (1971) Proc. Natl. Acad. Sci. (U.S.) 68, 1886–1890). A molecular weight of 0.15–3.0 × 106 daltons yields maximum formation of Ψ-DNA. Both the amplitude of the large negative CD band at 265 nm—a chief characteristic of the Ψ state—and the thermal stability of Ψ-DNA increase linearly with increasing mole fraction of guanine plus cytosine in the DNA sample. Either ethidium or proflavine, at concentrations where approximately one dye is bound per 5–10 nucleotide residues, can prevent the transition completely. Striking similarities between the Ψ-DNA produced by poly(ethylene oxide) + salt and the complexes formed between DNA and lysine-rich histone f1 suggest the presence of similar nucleic acid–nucleic acid interactions in both types of condensed phase.

The binding of ethidium bromide to DNA has been studied by various optical methods. From fluorescence polarization studies, and film, electric linear dichroism, and circular dichroism spectra, we propose assignments of the absorption bands of the dye, which are discussed in connection with wave-mechanical calculations recently reported. The optical activity induced in the dye absorption bands upon binding to DNA was attributed to various origins depending on the electronic transition considered. The visible absorption band displayed a circular dichroism due to the asymmetry of the binding site and independent of the amount of binding. The transition identified at 378 nm from the circular dichroism and electric dichroism observations was thought to be due to a magnetic-dipole transition. It remained constant with increasing amounts of dye bound. The main ultraviolet band showed circular dichroism characteristics corresponding to exciton interactions between dye molecules bound to neighboring sites. The electric dichroism observed for the strongly bound dye molecules indicated that the phenanthridinium ring of ethidium bromide was probably not perfectly parallel to the DNA base planes. When the amount of dye bound to DNA exceeded the maximum amount compatible with the exclusion of adjacent binding sites, the electric dichroism decreased owing to the appearance of externally bound dye molecules with no contribution to the dichroism. Sonicated DNA was used to study the lengthening of the DNA molecule upon complexation. Although the viscosity of the complexes increased with the amount of binding, the rotational diffusion coefficient measured by the electric birefringence relaxation was not detectably affected. The absence of variation in the electric birefringence with the binding indicated that the DNA base stacking remained unaltered.

The binding of ethidium bromide to calf thymus DNA is investigated over a wide range of temperatures and alcohol concentrations by means of fluorescence techniques. The presence of alcohol is found to lower the association constant, as isopropanol and n-propanol are more effective than ethanol and methanol. It is also found that the data from different alcohols fall very close on the same straight line when plotted vs the solution dielectric constant ϵ. It is shown that the dependence of the binding constant on ϵ is beyond the prediction of current polyelectrolyte theories; rather, it appears that the binding is greatly controlled by the activity coefficient of the dye. The thermodynamic functions of the reaction have been estimated by means of Van't Hoff analysis: a large, negative enthalpy contributes to the binding, whereas the entropy, also favorable, is only slightly responsible for the overall free energy. Both enthalpy and entropy are strong functions of temperature and alcohol concentration. We show that the dependence of the thermodynamic quantities on the temperature is removed by considering “isodielectric” binding. This can be accomplished by a proper choice of the alcohol concentration, so that the thermal dependence of ϵ is compensated. It is found that the isodielectric free energy, enthalpy, and entropy are the same for different alcohols when plotted vs ϵ. When looking at the isodielectric quantities, it appears that the binding is now opposed by a positive enthalpy, whereas the observed favorable free energy results mainly from a large and positive entropy. The relevance of hydrophobic effects emerges from the behavior of the isodielectric thermodynamic quantities, as well as from the similarities observed when other interacting systems are compared.

The conformation of DNA complexes formed with various 3-amino- and 3,8-diamino-phenanthridinium derivatives were examined by CD and fluorescence methods. The CD of these complexes is characterized by major bands in the 300–350-nm and the 400–550-nm regions. The CD properties of the complexes formed with diaminophenanthridinium derivatives suggest that the structure of such complexes is well represented by the intercalation complex formed between DNA and ethidium bromide. The substantial and regular increases in ellipticities near 308 nm that occur with increasing DNA-bound diaminophenanthridinium to DNA phosphate ratios (r) may result from direct interactions between molecules intercalated in neighbouring binding sites. In contrast, the changes in the shape of the CD of DNA complexes of monoaminophenanthridinium derivatives with r and the much lower maximum ellipticities attained suggest that near-neighbor interactions among intercalated monoaminophenanthridinium derivatives occur much less efficiently than in the corresponding diamino complexes, if at all. Although alternative explanations for the differences in the optical properties between the mono- and diaminophenanthridinium complexes of DNA may be offered, such results seem to indicate that complexes formed with monoaminophenanthridinium derivatives are characterized by a conformation which is quite distinct and different from that of the DNA–diaminophenanthridinium complexes. This conclusion is further supported by the considerable increase in fluorescence that accompanies the binding of the diaminophenanthridinium derivatives to DNA as compared to the minor increases, which occur upon the binding of the monoaminophenanthridinium compounds. The importance of conformation as a factor influencing template, function, especially with respect to the RNA polymerase-catalyzed synthesis of RNA, is now well appreciated. Therefore, methods which could provide information readily about changes in the conformation of a template, i.e., as a result of dye intercalation, are expected to facilitate our understanding of the effects of conformational change on the function and activity of templates.

Fluorescence correlation spectroscopy (FCS) and fluorescence photobleaching recovery (FPR) are two methods that may be used to measure diffusion and chemical reaction kinetics in small, labile systems such as biological cells. These methods are here applied to systems in which a fluorescent ligand can bind to a polyvalent substrate molecule in a multistep reaction sequence. The analytical theory for both FCS and FPR is extended to allow analysis of these kinds of systems. Experimental measurements of the binding of ethidium bromide to DNA by FCS confirm the theoretical analysis. (FPR measurements on the same system are reported in the accompanying paper.) The analysis shows that FCS and FPR perceive multivalent binding reactions differently. This difference results from the selective effect of the photobleaching process in the chemical reaction system. The development and results we report could have useful applications to a wide range of biopolymeric binding and assembly process.

A self-consistent thermodynamic characterization of the binding of ethidium to yeast phenylalanine-specific tRNA at 25°C, pH 7.0, in 11 nM MgCl2, 375 nM NaCl, and 25 mM sodium phosphate has been obtained. Two ethidium molecules bind per tRNA under these conditions. The stronger site has a dissociation constant equal to 1.9 ± 0.5 μM and ΔHdis°′ = 12 ± 1 Kcal/mol, and the weaker sites has a dissociation constant equal to 24 ± 9 μM and ΔHdis°′ = 8.9 ± 1.5 Kcal/mol. The average calorimetric ΔHdis°′ for the to sites 10.6 ± 0.4 kcal/mol. The thermodynamics of binding to the stranger sites are most probably the thermodynamics of interaction between A·U (6) and A·U (7), the unique site identified by Jones and Kearns. The binding is enthalpically driven and classical hydrophobic interactions do not appear to be important in the binding reaction.

The equilibrium binding of ethidium bromide (EB) to two small 147 base-pair (bp) DNA restriction fragments, which exhibit different mobilities in polyacrylamide gels, was investigated by CD. Two larger DNA restriction fragments and calf thymus DNA were also studied for comparison. Difference spectra were calculated by subtracting the spectrum of the pure DNA from the spectra of its DNA–EB complexes. The D/P ratios ranged from 0.03 to 1.0. The difference CD spectra of all fragments are characterized by bands with maxima near 310, 275, and 207 nm, and minima near 290, 253, 225, and 190 nm. The band near 310 nm, which has a shoulder at about 335 nm, has zero intensity at D/P ≤ 0.05, and rises to a plateau value, different for each fragment, at D/P ≃ 0.3 for large fragments (≥ 1400 bp), and D/P ∼ 0.7 for the two small 147 bp fragments. The minimum near 290 nm is markedly blue shifted with increasing D/P, the wavelength of the extremum corresponding approximately to the wavelength of the uv absorption maximum of the DNA–EB complex. The negative amplitude of this band at D/P = 1.0 depends on the molecular weight of the DNA. The difference CD maximum near 275 nm is positive at low D/P ratios, increases and goes through a maximum at D/P = 0.06–0.1, and then becomes increasingly negative with increasing D/P. The amplitude of the negative ellipticity per added dye is constant at high D/P ratios, suggesting that the transition can be attributed to outside-bound EB molecules. The ellipticities at 310, 290, and 253 nm increase in absolute magnitude with increasing D/P at approximately the same rate, suggesting that all three bands are associated with the same optical and/or conformational transition. For the two small 147 bp fragments the fractional increases in amplitude of these bands parallel the fractional increase in length of the DNA upon binding EB, determined by electric birefringence measurements. The titration of the restriction fragments with EB was also followed by optical absorption. Two end points are observed, the first at a D/P ratio of ∼ 0.1, reflecting the transition between intercalated and outside-bound dye molecules, and the second at D/P ≃ 1.0, the equivalence point of the titration.

The enthalpy ΔH for the intercalation of the ethidium cation (EC) into DNA minihelices can be decomposed into (1) an energy of conformational adjustment (i.e., the energy of minihelix extension and unwinding from the B-form to the intercalated form) and (2) EC minihelix intermolecular interactions. In the present study, we have focused our attention mainly on a decomposition of the energetic factors of the EC minihelix intermolecular interactions, while the essential features of the energy of conformational adjustment have been discussed in detail elsewhere by us. The structural features of the various resulting energy-minimized EC-intercalated complexes are compared with each other and the initial x-ray model structure. ΔH is estimated to be in the range of −12.3 to −24.0 kcal/mol. This theoretical estimate is qualitatively and quantitatively in agreement with a variety of available experimental data. The energy of conformational adjustment is an energetically unfavorable step, while the energetically favorable contribution of the EC minihelix intermolecular interactions is responsible for the overall favorable nature of the intercalation process involving the EC. On the other hand, the observed preference for intercalation into Pyr(3′–5′)Pur DNA sequences over their isomeric Pur(3′–5′)Pyr sequences is controlled by the energy of conformational adjustment and not by the EC minihelix intermolecular interaction contribution. No base-composition effect is expected at EC concentrations normally found at cellular conditions. Moreover, the structural features of the various EC-intercalated complexes are very similar regardless of minihelix base sequence or composition. These results compare favorably with available evidence. The nature of biologically preferred sites of EC binding with the minihelices is discussed.

The relaxation kinetics of binding of ethidium to calf-thymus DNA as studied previously by the temperature-jump method with absorption detection [Bresloff, J. & Crothers, D. M. (1975) J. Mol. Biol.95, 103] is reanalyzed in terms of a series of models for DNA-ligand interactions that include cases with and without internal and bimolecular direct transfer of ligands between different binding modes or different binding sites. The experimental results are shown to be consistent with two alternative binding mechanisms. Both models include bimolecular “direct transfer” steps and a site size of two base pairs per site. In the first model, there exist two distinct modes of binding to the DNA double helix at each binding site. In the second model, sites containing at least one GC base pair constitute a different and stronger class of binding sites than those containing only AT base pairs. The existence of a direct transfer pathway between two classes of bound ligands is supported by the linear increase of reciprocal relaxation times far beyond the concentration regions, where off-rates should have become rate limiting. The second model, incorporating the notion of base selectivity, is in quantitative agreement with published work on ethidium binding to DNAs of different base compositions and with nmr measurements of bound ligand lifetimes.

The rate of renaturation of T2 DNA has been studied as a fuction of ethidium bound per nucleotide of denatured DNA. The Binding constants and number of binding sites for ethidium have been determined by spectral titration for denatured DNA at 55, 65, and 75°C and for native DNA at 65°C in 0.4M Na+. The rate of renaturation of T2 DNA was found to be independentof ethidium binding up to 0.03 moles per mole of nucleotide. Above 0.03 moles, the rate drops off precipitously approaching zero at 0.08 and 0.06 moles bound ethidium per nucleotide at 65°C respectively. A study was also made of the use of bound ethidium fluorescence as a probe for monitoring DNA renaturation reactions.

synopsis This paper describes the first experimental application of fluorescence correlation spectroscopy, a new method for determining chemical kinetic constants and diffusion coefficients. These quantities are measured by observing the time behavior of the tiny concentration fluctuations which occur spontaneously in the reaction system even when it is in equilibrium. The equilibrium of the system is not disturbed during the experiment. The diffusion coefficients and chemical rate constants which determine the average time behavior of these spontaneous fluctuations are the same as those sought by more conventional methods including temperature-jump or other perturbation tecliniques. The experiment consists essentially in measuring the variation with time of the number of molecules of specified reactants in a defined open volume of solution. The concentration of a reactant is measured by its fluorescence; the sample volume is defined by a focused laser beam which excites the fluorescence. The fluorescent emission fluctuates in proportion with the changes in the number of fluorescent molecules as they diffuse into and out of the sample volume and as they are created or eliminated by the chemical reactions. The number of these reactant molecules must be small to permit detection of the concentration fluctuations. Hence the sample volume is small (10-8 rnl) and the concentration of the solutes is low (-10-9 M). We have applied this technique to the study of two prototype systems: the simple example of pure diffusion of a single fluorescent species, rhodamine 6G, and the more interesting but more challenging example of the reaction of macromolecular DNA with the drug ethidium bromide to form a fluorescent complex. The increase of the fluorescence of the ethidium bromide upon formation of the complex permits the observation of the decay of concentration fluctuations via the chemical reaction and consequently the determination of chemical rate constants.

The pKa of 3,8-diamino-6-phenyl-phenanthridine (DAPP), a nonquaternary analog of ethidium bromide, has been determined spectrophotometrically as a function of sodium ion concentration both free in solution and complexed to DNA. Unwinding angle determinations with this compound were determined with Col El DNA using ethidium bromide as a standard. The unwinding angle for DAPP was 24 ± 2° relative to 26° for ethidium, and this suggests that DAPP binds in a manner quite similar to ethidium and with no significant outside bound DAPP under these experimental conditions. Isobestic behavior was obtained on spectrophotometric pH titration above pH 5 as long as the ratio of DNA-phosphate to ligand was between 100 and 300 and the DNA phosphate concentration was approximately 0.01M or greater. The loss of isosbestic behavior which occurred below pH 5 is probably due to titration of the 8 amino group of the ligand complexed to DNA. To circumvent this problem, pKa values and the extinction coefficient of the acidic species were both determined by a computer program using experimental data obtained above pH 5. The pKa of the free compound has only a minor dependence on ionic strength, while the pKa of the ligand bound to DNA in an intercalated complex depends strongly on the sodium ion concentration. The pKa of the DAPP-DNA complex is a linear function of –log[Na+] as predicted by the ion-condensation theory of polyelectrolytes. It was determined that DAPP is essentially completely bound to DNA under the conditions of these experiments by (1) determination of apparent pKa values as a function of total DNA concentration, (2) calculation of binding constants for the neutral species of DAPP, and (3) spectral analysis of the protonated and neutral species of DAPP bound to DNA relative to DAPP free in solution. These results support the ion-condensation theory; provide an independent method for measuring ψ*, the average number of counterions associated per phosphate of DNA in the intercalated conformation; and illustrate that there are no specific pH effects or absolute pKa values for ligands bound to DNA, but only ionic-strength-dependent results.

The preceding paper develops the theory for the interpretation of fluorescence photobleaching recovery (FPR) measurements of multiple binding of a ligand to a multivalent substrate molecule. Based on a reasonable assumption about the mechanism of the photobleaching process, this analysis shows that the observed behavior of a multivalent system should be practically identical to that of a univalent binding system. This is in contrast to the expected and observed behavior of fluorescence correlation spectroscopy (FCS) measurments. Experimental FPR measurements of multivalent binding of ethidium bromide to DNA confirm these conclusions. The FCS and FPR measurements also reveal an apparently enhanced diffusion of ethidium at high DNA concentration. This enhancement might result from direct transfer of ethidium among DNA molecules.

The orientation of ethidium dye in DNA and the amplitude of its local internal angular motion are estimated from fluorescence polarization anisotropy and reduced linear dichroism data. When the local internal motion is assumed to be isotropic, the acceptable range of polar angles of the transition dipole is ϵ = 70°−72°, and the acceptable range of root mean squared (rms) amplitudes of local internal motion is 〈δϵ2〉1/2 = 6.9°–8°, in agreement with earlier estimates. The nmr relaxation data reported by Kearns and co-workers for the imino protons of duplex (dAdT)26.5 and (dGdC)30 are analyzed using recent theoretical results for flexible filaments. For typical, or reasonable, assumed geometrical parameters, large rms amplitudes of local internal motion of the bases are not required to be superimposed on the collective motions due to twisting and bending deformations. For the particular geometrical parameters considered herein, rms amplitudes greater than about 12° are precluded by the data, but values as low as 0° are not. The low precision of present knowledge about solution structures does not allow a definitive statement about the rms amplitudes of local angular motion of the bases to be made independent of any structural or geometric assumptions.

PM2 DNA molecules were treated with intercalating reagents (ethidium bromide, ethidium dimer, acridine dimer) and observed by electron microscopy. The adaptation of different electron microscopy techniques has enabled the determination of DNA lengthening upon drug intercalation. A 50% length increase was generally obtained for DNA saturated with the drugs. This result is in agreement with the intercalation model proposed by Lerman. In some cases (ethidium dimer), an increase of length larger than 50% can be obtained. Experimental conditions of DNA spreading strongly interfere with the DNA–drug interaction. In some cases it was possible to estimate the apparent binding constants and also to distinguish the mono- from the bisintercalating derivatives in their reaction with DNA.

A time-resolved fluorescence study of ethidium bromide (EB) in the presence of poly(dG-dC) and of poly(dG-dC) modified by chlorodiethylenetriamine platinum(II) chloride is presented under solvent conditions in which these polymers adopt the Z-conformation (high ionic strength). It is shown that these polynucleotides can intercalate a very small quantity of EB. The binding parameters have been determined. The fluorescence lifetime of EB is slightly higher when bound to the Z-conformation (≃25 ns) than when bound to the B-conformation (≃23.7 ns). The nature of the salt has been checked. In the presence of 2.5M NaClO4, no transition from the Z-conformation to another conformation is observed when EB is added. On the contrary, in the presence of 4.25M NaCl, EB induces a cooperative transition from the Z-conformation to a conformation characterized by a much higher affinity for EB intercalation. In the case of poly(dG-dC) this last conformation is identical to the one observed at low ionic strength (B-conformation), but in the case of the platinated polymer this conformation is slightly different, as judged by the smaller value of the fluorescence lifetime of the intercalated EB.

Time resolved x-ray solution scattering measurements were made during thermal denaturation of DNA from various sources in the temperature range of 20-90 degrees C. Preliminary results on the influence of fragment length, ionic strength, and origin of the DNA on the time course of the scattering are described. Interpretation is based on model calculations of the scattering patterns. The results indicate that, for long DNA fragments at very low ionic strength, the melting process is a continuous phenomenon over the whole temperature range. It is accompanied by a progressive decrease of the radius of gyration of the cross section and of the mass per unit length. For short fragments of 146 base pair nucleosomal core DNA, stiffening of the DNA appears to precede a sharp melting transition.

We have measured the specific viscosity of closed circular PM2 DNA in the presence of concentrations of ethidium bromide ranging up to 5 mg/ml. Both native viral PM2 DNA I and enzymatically prepared relaxed, closed circular PM2 DNA I0 exhibit a complex dependence of the specific viscosity upon the extent of supercoiling. As the number of superhelical turns is increased in the positive sense from zero, the viscosity first decreases to a minimum, then passes through a secondary maximum, and eventually again increases as the dye-induced duplex unwinding proceeds. In the case of DNA I, a corresponding behavior is mirrored in the negative sense as dye is removed from the principal viscometric maximum (complete relaxation of the DNA by dye). The shape of the curve relating specific viscosity to extent to supercoiling is similar for superhelical DNAs of either handedness, a result which we interpret to mean that the influence of any regions of special secondary structure (such as denatured loops) upon the viscosity is minimal. At very high dye concentrations the specific viscosity decreases dramatically. This effect might arise either from intermolecular aggregation or from a dye-induced collapse in the DNA secondary structure.

Covalently closed intracellular DNA obtained from Pseudomonas BAL 31 20 min after infection with PM2 phage has been shown to be heterogeneous in superhelix density. Analytical band sedimentation, in the presence of low concentrations of ethidium bromide, has been carried out on fractions centripetal and centrifugal to the mode of a single band of closed circular DNA in a preparative propidium iodide–CsCl buoyant density gradient. Different average sedimentation rates, as well as different band shapes, have been observed for upper and lower fractions centrifuged at a dye concentration near the minimum in s° versus ethidium bromide concentration titrations performed on DNA from proximate intermediate fractions. Similar differences, although not as pronounced, have been obtained at a dye concentration corresponding to a point in the steep region of the titrations. Differential band sedimentation experiments performed on the same fractions have confirmed these results. Differential band sedimentation experiments on similarly fractionated mature PM2 I DNA (closed circular form) have shown slight differences in the relative sedimentation rates of upper and lower fractions at dye concentrations corresponding to the steep regions in the titrations. The same experiments, when performed on nicked circular DNA obtained from heating both the mature and intracellular fractions, showed no evidence of differences in sedimentation coefficients. Such results may indicate slight heterogeneity in the superhelix density of viral PM2 I DNA; however, the degree of this heterogeneity would be somewhat less than that of the intracellular DNA. The possibility that superhelix density heterogeneity may arise from displacement loops, which have been found at low levels in intracellular PM2 DNA, has been subjected to experimental tests. Unless such structures are originally present and removed by the isolation procedure, this possibility may be rejected.

Several intercalating dyes are shown to inhibit the cation-induced condensation of λ-DNA when Co3+(NH3)6 is the condensing agent. The dyes that have been studied are ethidium, propidium, proflavin, quinacrine, and actinomycin D. Earlier work has shown that intercalating dyes inhibit ψ-DNA condensation. [Lerman, L. S. (1971) Prog. Mol. Subcell. Biol.2, 382–391; Cheng, S. & Mohr, S. C. (1975) Biopolymers14, 663–674.] Dye-induced decondensation of intramolecularly condensed DNA has been studied by making use of conditions in which Co3+(NH3)6 produces intramolecular condensation without significant aggregation. Some aggregation is caused, however, during dye-induced decondensation. Dye titration curves of DNA decondensation have been measured by excess light scattering to monitor decondensation and by fluorescence to monitor intercalation. All of the dyes studied act as competing cations in displacing the condensing cation Co3+(NH3)6 from the DNA. Competition occurs both in and below the transition zone for condensation. The effectiveness of a dye as a competing cation increases with its net positive charge. Before decondensation begins, no intercalated dye can be detected, suggesting that intercalation might be incompatible with the proper helix packing needed for cation-induced DNA condensation. To test this last point, methidium–spermine was synthesized: it contains an intercalating methidium head group combined with a polyamine tail. Methidium–spermine is found to cause λ-DNA condensation, but aggregation accompanies condensation, as has been found earlier for spermine and spermidine. Fluorescence and absorption spectra indicate that the methidium group is intercalated when the DNA is condensed, indicating that intercalation need not be incompatible with DNA condensation. The presence of aggregates among the condensed DNA molecules makes this last conclusion tentative.

The thermodynamics of ethidium ion binding to the double strands formed by the ribooligonucleotides rCA5G + rCU5G and the analogous deoxyribo-oligonucleotides dCA5G + dCT5G were determined by monitoring the absorbance versus temperature at 260 and 283 nm at several concentrations of oligonucleotides and ethidium bromide. A maximum of three ethidium ions bind to the oligonucleotides, which is consistent with intercalation and nearest-neighbor exclusion. For the ribo-oligonucleotide the binding mechanism is complex. Either two sites (assumed to be the intercalation sites at the two ends of the oligonucleotide) bind more strongly by a factor of 140 than the third site, or all sites are identical, but there is strong anticooperativity on binding (cooperativity parameter, 0.1). In sharp contrast, the binding to the same sequence (with thymine substituted for uracil) in the deoxyribo-oligonucleotide showed all sites equivalent and no cooperativity. For the ribo-oligonucleotides the enthalpy for ethidium binding is −14 kcal/mol. The equilibrium constants at 25°C depend on the model; either K = 6 × 105M−1 for the two strong sites (4 × 103M−1 for the weak site) or K = 2.5 × 105M−1 for the intrinsic constant of the anticooperative model. For the equivalent deoxyribo-oligonucleotide the enthalpy of binding is -9 kcal/mol and the equilibrium constant at 25°C is a factor of 10 smaller (K = 2.5 × 104M−1).

Vibrational normal mode calculations are presented for a DNA hexanucleoside pentaphosphate, d(CpGpCpGpCpG)2, and for its complex with the cationic intercalator ethidium. Two intercalation sites are modeled that differ in DNA backbone torsion angles. Normal mode frequencies for the DNA fragment itself are significantly lower than those reported earlier using different force fields, but an analysis of "effective" frequencies suggests that somewhat higher frequencies are more appropriate. Intercalation leads to significant lowering of mobility for the base pairs adjacent to the drug; in this sequence, the ethidium binding affects the guanosine atoms more strongly than the cytosine atoms. Motions of the bases and the intercalator are analyzed in terms of "twist" about the local helix axis and a "tilt" angle relative to this axis, and the results are compared to fluorescence studies of ethidium-DNA complexes.

Molecular mechanical calculations were done on complexes of ethidium cation with various base-paired deoxydinucleoside monophosphates [(ApT)2, (TpA)2, (A2 · T2), (GpC)2, (CpG)2, and (G2 · C2)] and deoxyhexanucleoside pentaphosphates [(ATATAT)2, (TATATA)2, (A6 · T6), (GCGCGC)2, (CGCGCG)2, and G6 · C6]. Relative binding energies, sequence preferences, and conformational aspects of the intercalation complexes were studied. The most detailed models used (an all-atom force field) gave results in good agreement with previous calculations and experimental work. Less-sophisticated models did not perform as well.

The binding of methylene blue, proflavine, and ethidium bromide with DNA has been studied by spectrophotometric titration. Methylene blue and proflavine or methylene blue and ethidium bromide were simultaneously titrated by DNA. The results indicate that all of these dyes compete for the same bindine sites. The binding properties are discussed in terms of symmetry. The optical properties of the dye–DNA complexes have been studied as a function of DNA/dye ratio. The induced circular dichriosm due to dye–dye interaction was measured at low dye/DNA ratios for cases involving both the same dye and different dyes. A positive Cotton effect for DNA–proflavine complex may be induced at 465 mμ by eithr proflavine or ethidium bromide, whereas a netgative Cotton effect at 465 mμ may be induced by methylene blue. The limiting circular dichroism, with no dye–dye interaction, and the induced circular dichroism spectra are discussed in terms of symmetry rules.