Ligand-induced DNA condensation: choosing the model

We test and compare different models for ligand-induced DNA condensation. Using 14C-labeled spermidine3+, we measure the binding to condensed DNA at micromolar to molar polyamine concentrations. DNA aggregates at a critical polyamine concentration. Spermidine3+ binding becomes highly cooperative at the onset of aggregation. At higher concentrations, spermidine3+ binding to condensed DNA reaches a plateau with the degree of binding equal to 0.7 (NH(4+)/PO3-). Condensed DNA exists in a wide range of spermidine concentrations with the roughly constant degree of ligand binding. At greater concentrations, the degree of binding increases again. Further spermidine penetration between the double helices causes DNA resolubilization. We show that a simple two-state model without ligand-ligand interactions qualitatively predicts the reentrant aggregation-resolubilization behavior and the dependence on the ligand, Na+, and DNA concentrations. However, such models are inconsistent with the cooperative ligand binding to condensed DNA. Including the contact or long-range ligand-ligand interactions improves the coincidence with the experiments, if binding to condensed DNA is slightly more cooperative than to the starting DNA. For example, in the contact interaction model it is equivalent to an additional McGhee-von Hippel cooperativity parameter of approximately 2. Possible physical mechanisms for the observed cooperativity of ligand binding are discussed.     

Analysis of distribution of ligands adsorbed on DNA fragments

The effect of finite fragment length on the distribution pattern of bound protein along the DNA fragment is considered. If the size of the binding site for a ligand on DNA is comparable with the length of the DNA fragment fluctuations in the amount of ligand bound to the fragment create some difficulties for evaluating the distribution pattern of ligand on DNA. A mathematical approach is developed which enables one to calculate the distribution pattern of ligand on DNA provided that the number of bound ligand on the DNA fragment is known. Expression are also obtained to treat the effects of fluctuations in the number of ligand molecules bound to the DNA fragment on the distribution pattern of ligand. A new procedure is proposed which may be useful for locating the preferable binding sites for ligand on DNA on the basis of footprinting experiments.     

Enthalpy/entropy compensation: influence of DNA flanking sequence on the binding of 7-amino actinomycin D to its primary binding site in short DNA duplexes

The effect of the context of the flanking sequence on ligand binding to DNA oligonucleotides that contain consensus binding sites was investigated for the binding of the intercalator 7-amino actinomycin D. Seven self-complementary DNA oligomers each containing a centrally located primary binding site, 5'-A-G-C-T-3', flanked on either side by the sequences (AT)(n) or (AA)(n) (with n = 2, 3, 4) and AA(AT)(2), were studied. For different flanking sequences, (AA)(n)-series or (AT)(n)-series, differential fluorescence enhancements of the ligand due to binding were observed. Thermodynamic studies indicated that the flanking sequences not only affected DNA stability and secondary structure but also modulated ligand binding to the primary binding site. The magnitude of the ligand binding affinity to the primary site was inversely related to the sequence dependent stability. The enthalpy of ligand binding was directly measured by isothermal titration calorimetry, and this made it possible to parse the binding free energy into its energetic and entropic terms. Our results reveal a pronounced enthalpy-entropy compensation for 7-amino actinomycin D binding to this family of oligonucleotides and suggest that the DNA sequences flanking the primary binding site can strongly influence ligand recognition of specific sites on target DNA molecules.     

DNA interaction with low molecular ligands of different structure. II. Complexes of DNA with actinomine and its analogs

DNA-complexes with actinomine and its analogues containing omega-dialkylaminoalkyl groups at 1,9 positions of the phenoxazone moiety were studied by technique of spectrophotometry, viscometry and flow birefringence. In the process of spectrophotometry titration two groups of spectra corresponding to different DNA--ligand ratio in a complex were observed. According to the experimental data the investigated compounds are bounded to DNA by means of intercalation and external binding. There within a region of low degrees of binding the intercalation type of the ligand--DNA interaction prevails. In virtue of the spectrophotometry data the intercalation binding share was calculated. The intrinsic viscosity of a complex increases in the case of ligand intercalation and does not change as it joins to the DNA double-helix from outside. Optical anisotropy of DNA molecule increases linearly irrespective of the way of ligand binding. Data on the flow birefringence permits to conclude that under external binding the angle between the normal to the ligand chromophore plane and the axis of DNA double-helix is about zero. During ligand intercalation the equilibrium rigidity of DNA molecules increases.     

Quantifying force-dependent and zero-force DNA intercalation by single-molecule stretching

We used single DNA molecule stretching to investigate DNA intercalation by ethidium and three ruthenium complexes. By measuring ligand-induced DNA elongation at different ligand concentrations, we determined the binding constant and site size as a function of force. Both quantities depend strongly on force and, in the limit of zero force, converge to the known bulk solution values, when available. This approach allowed us to distinguish the intercalative mode of ligand binding from other binding modes and allowed characterization of intercalation with binding constants ranging over almost six orders of magnitude, including ligands that do not intercalate under experimentally accessible solution conditions. As ligand concentration increased, the DNA stretching curves saturated at the maximum amount of ligand intercalation. The results showed that the applied force partially relieves normal intercalation constraints. We also characterized the flexibility of intercalator-saturated dsDNA for the first time.     

Cooperation effects in binding of large ligands to DNA. II. Contact interactions between adsorbed ligands

Cooperative effects arising upon binding of biologically active ligands to DNA are considered. Equations are derived which enable one to describe the binding of two different ligands to DNA. We also consider the case when ligand can form two type of DNA complexes. The cooperative binding of the ligand in the vicinity of saturation level of binding can be described with a good accuracy by equation derived for the non-cooperative adsorption of the same ligand with some effective binding constant Keff. It is shown that cooperative effects arising upon binding of proteins and other ligands to DNA can be divided into two groups depending on the symmetry of interactions between the bound ligand molecules. In particular, if such interactions favor the formation of dimeric ligand species on the DNA, Keff approximately a1/2, where a is the ligand-ligand interaction constant. If cooperative interactions favor the formation of aggregates of unrestricted size, then Keff approximately aL+Y, where L is the size of the binding site for the ligand on DNA.     

92 Novel interpretation of the isotherms of multimodal ligands binding with DNA

The binding of ligands with DNA is a key moment in a whole range of cellular processes that provide not only the normal cell vital activity but also the development of some pathological processes. Depending on ligand type, structure of DNA adsorption centers, and physical–chemical conditions of the surrounding, the ligand may bind to DNA by several modes [1]. Particularly, adsorption isotherm of multimodal ligands binding to DNA in Scatchard’s coordinates has a concave shape with two brightly expressed linear areas in the region of small fillings. The analysis of such type of adsorption isotherm for determining of important binding parameters such as binding constant and number of adsorption centers (the part of DNA polymer with which one ligand molecule binds) presents difficulties. Practically in all cases, the analysis of such adsorption isotherm is carried out by linear parts of curves. Such analysis mode of experimental points is approximate method, since all registered of experimental points are roughly divided into two groups and they are treated by linear binding isotherm and therefore the binding parameters are determined. In the present work, the non-linear adsorption isotherm in Scatchard‘s coordinates is obtained which allowed, provided, the more precise treatment of all experimental points by unique curve which includes linear regions as well. Such mode of treatment of experimental points makes more precise the determination of not only binding constant and number of adsorption centers that correspond to the one ligand molecule binding, but also additional binding parameter – a proportion of adsorption centers of each binding to DNA type of multimodal ligand.     

A polarized-light spectroscopy study of interactions of a hairpin polyamide with DNA

We here study the interactions of a polyamide with large DNA, and compare to those of minor groove binder distamycin (DST), including high ligand/DNA binding ratios. Specific as well as nonspecific binding is probed using polarized-light spectroscopy combined with singular value decomposition analysis. Circular and linear dichroism data confirm binding geometries consistent with minor groove binding for both of the ligands. Interestingly, at high and intermediate ligand/DNA ratios the polyamide exhibits no significant sequence discrimination between mixed-sequence (calf thymus) and AT DNA as compared to DST. Each ligand is concluded to exhibit two different binding modes depending upon ligand/DNA ratio and nucleo-base sequence. At high binding ratios, distinct differences between the ligands are observed: circular dichroism spectra exciton effects provide evidence of bimolecular interactions of the polyamide when bound to AT-DNA, whereas no effects are seen with DST or mixed-sequence DNA. Also linear dichroism indicates that a change in binding geometry occurs at high polyamide/AT ratios, and that the effect occurs only with polyamide in contrast to DST. Since the effect is insignificant with DST, or with calf thymus DNA, it is concluded that it relates to the sizes of the ligands and the minor grooves, becoming critical in the limit of crowding.     

Calculations of DNA Condensation Caused by Ligand Adsorption

A method for calculating the curves of DNA transition from linear to condensed state upon binding of condensing ligands has been developed. The character of the transition and ligand concentration necessary for condensation have been shown to be governed by the length of DNA molecule, energy and stoichiometry parameters of the DNA–ligand complex (equilibrium constant between linear and condensed form in the absence of ligands, constants for ligand binding to linear and condensed forms, the number of base pairs covered by one ligand, etc.). The results of the calculations indicate that a slight difference in the free energies of these DNA states (less than 6 cal/mol(bp) for a DNA of 500 bp) is sufficient for the existence of a stable linear state in the absence of ligands (in free DNA) and the formation of stable condensed state upon complexation.     

Triostin A derived hybrid for simultaneous DNA binding and metal coordination

The natural product triostin A is known as an antibiotic based on specific DNA recognition. Structurally, a bicyclic depsipeptide backbone provides a well-defined scaffold preorganizing the recognition motifs for bisintercalation. Replacing the intercalating quinoxaline moieties of triostin A by nucleobases results in a potential major groove binder. The functionalization of this DNA binding triostin A analog with a metal binding ligand system is reported, thereby generating a hybrid molecule with DNA binding and metal coordinating capability. Transition metal ions can be placed in close proximity to dsDNA by means of non-covalent interactions. The synthesis of the nucleobase-modified triostin A analog is described containing a propargylglycine for later attachment of the ligand by click-chemistry. As ligand, two [1,4,7]triazacyclononane rings were bridged by a phenol. Formation of the proposed binuclear zinc complex was confirmed for the ligand and the triostin A analog/ligand construct by high-resolution mass spectrometry. The complex as well as the respective hybrid led to stabilization of dsDNA, thus implying that metal complexation and DNA binding are independent processes.     

DNA shuffling method for generating estrogen receptor alpha and beta chimeras in yeast

To facilitate our study of the molecular basis for the estrogen receptor (ER) subtype selectivity of novel ligands, we used DNA shuffling to construct chimeric ERs having ligand binding domains derived from both ER alpha and ER beta. The efficiency of chimera generation was low with traditional DNA shuffling protocols. Furthermore, ER ligand binding domain sequences lack convenient restriction sites for introducing chimeric ligand binding domain sequences into expression vectors. To overcome these problems, we developed a modified strategy whereby chimeric sequences were exclusively amplified from among the reassembled products from DNA shuffling using a special pair of PCR primers whose 3' ends specifically match the alpha and beta sequences, respectively, and whose 5' ends match sequences outside the ER beta ligand binding domain. When chimeric ligand binding domain DNA sequences, amplified with these primers, were co-transformed into a yeast strain with a linearized expression vector for ER beta, an active expression vector was produced by homologous recombination. Twenty-two different crossover sites were found; most occurred when there was a stretch of eight or more identical base pairs in both sequences, and many were concentrated in the regions important for studying ligand binding and transactivation. This method should prove to be useful for generating chimeric gene products from parent templates that share relatively low sequence identity.     

DNA sequence recognition by an isopropyl substituted thiazole polyamide

We have used DNA footprinting and fluorescence melting experiments to study the sequence-specific binding of a novel minor groove binding ligand (thiazotropsin A), containing an isopropyl substituted thiazole polyamide, to DNA. In one fragment, which contains every tetranucleotide sequence, sub-micromolar concentrations of the ligand generate a single footprint at the sequence ACTAGT. This sequence preference is confirmed in melting experiments with fluorescently labelled oligonucleotides. Experiments with DNA fragments that contain variants of this sequence suggest that the ligand also binds, with slightly lower affinity, to sequences of the type XCYRGZ, where X is any base except C, and Z is any base except G.     

Binding of symmetrical cyanine dyes into the DNA minor groove

Optical methods, such as fluorescence, circular dichroism and linear flow dichroism, were used to study the binding to DNA of four symmetrical cyanine dyes, each consisting of two identical quinoline, benzthiazole, indole, or benzoxazole fragments connected by a trimethine bridge. The ligands were shown to form a monomer type complex into the DNA minor groove. The complex of quinoline-containing ligand with calf thymus DNA appeared to be the most resistant to ionic strength, and it did not dissociate completely even in 1 M NaCl. Binding of cyanine dyes to DNA could also be characterized by possibility to form ligand dimers into the DNA minor groove, by slight preference of binding to AT pairs, as well as by possible intercalation between base pairs of poly(dG)-poly(dC). The correlation found between the binding constants to DNA and the extent of cyanine dyes hydrophobicity estimated as the n-octanol/water partition coefficient is indicative of a significant role of hydrophobic interactions for the ligand binding into the DNA minor groove.     

Modeling of DNA condensation and decondensation caused by ligand binding

A theoretical method for computer modeling of DNA condensation caused by ligand binding is developed. In the method, starting (s) and condensed (c) states are characterized by different free energies for ligand free DNA (F(s) and F(c) respectively), ligand binding constants (K(s) and K(c)) and stoichiometry dependent parameters (c(sm) and c(cm) - maximum relative concentration of bound ligands (per base pair) for starting and condensed state respectively). The method allows computation of the dependence of the degree of condensation (the fraction of condensed DNA molecules) on ligand concentration. Calculations demonstrate that condensation transition occurs under an increase in ligand concentration if F(s) < F(c) (i.e. S(sc) = exp [- (F(c) - F(s)) / (RT)], the equilibrium constant of the s-c transition, is low (S(sc) < 1)) and K(s) < K(c). It was also found that condensation is followed by decondensation at high ligand concentration if the condensed DNA state provides the number of sites for ligand binding less than the starting state (c(sm) > c(cm)). A similar condensation-decondensation effect was found in recent experimental studies. We propose its simple explanation.     

Calculation of DNA condensation, caused by adsorption of ligands

A method for calculating the curves of DNA transition from linear to condensed state upon binding of condensing ligands has been developed. The character of the transition and ligand concentration necessary for condensation have been shown to be governed by the length of DNA molecule, energy and stoichiometry parameters of DNA-ligand complex (equilibrium constant between linear and condensed form in the absence of ligands, constants for ligand binding to linear and condensed forms, the number of base pairs covered by one ligand, etc.). The results of the calculations indicate that only slight difference in the free energies of these states in free DNA (less than 6 cal/mole(bp) for DNA of 500 bp long) is sufficient for the existence of stable linear state in the absence of ligands (in free DNA) and the formation of stable condensed state upon complexation.     

Effect of ligand binding on the buoyant density of DNA in Nycodenz gradients.

The effect of ligand binding upon the buoyant density of DNA in Nycodenz gradients has been studied using DNAs of differing base compositions. The effect of both intercalating ligands (ethidium bromide and proflavin) and non-intercalating ligands (distamycin A, DAPI and netropsin) has been studied. The binding of intercalating ligands to DNA has essentially no effect on the buoyant density of DNA in Nycodenz gradients. The non-intercalating ligands were found to increase the buoyant density of DNA in a base specific manner. The increase in buoyant density can be interpreted in terms of disruption of the hydration shell of the DNA molecule caused by the binding of the ligand along the minor groove of the DNA helix.     

Multimode Interaction of Hoechst 33258 with Eukaryotic DNA; Quantitative Analysis of the DNA Conformational Changes

Abstract

The interaction of the minor groove binding ligand Hoechst 33258 (Hoe) with natural DNA was investigated by high resolution titration rotational viscometry. Analysis of the concomitant DNA conformational changes was performed with two DNA samples of sufficiently different molar mass M, at 4°C, 22°C and 40°C, for Hoe/DNA-P ratios below r = 0.02. In this narrow r range several interaction modes could be resolved. The measured conformational changes were quantified in terms of relative changes of both apparent DNA persistence length, Δa/a, and hydrodynamically operative DNA contour length, ΔL/L. Δa/a(r) primarily is a measure of ligand-induced DNA helix stiffening, but both, Δa/a(r) and ΔL/L(r), generally depend also on ligand binding induced DNA bending or DNA unbending. The essential difference obviously is that Δa/a(r) is influenced by the randomly distributed helix bends and ΔL/L(r) by phased ones. The measurements performed at different temperatures deliver informations about existence and temperature dependent abolition of intrinsic helix curvature.

Both Hoe and netropsin (Nt) prefer binding to AT rich DNA segments, which are candidates for intrinsic DNA helix bends. But our data for Hoe interaction with calf thymus DNA (ctDNA) show characteristic differences to those for Nt-ctDNA interaction. Especially for Hoe, the mode of highest affinity is saturated already at a ligand concentration of roughly 1 nM (r = 0.0015 Hoe/DNA-P). It exhibits an unusually strong temperature dependence of the conformational DNA response. A Hoe-Nt competition experiment shows that Hoe binding to the sites of the very first Hoe mode is almost unaffected by bound Nt. But Hoe binding to the sites of the following Hoe modes does not occur due to the competition with Nt. Thus this mode of strongest Hoe-DNA interaction reflects a unique mechanism, possibly of high relevance for gene regulatory systems.