Structure of a DNA intercalation complex as determined by NMR using a paramagnetic probe

Longitudinal relaxation rates of the protons of the 3,8-dimethyl-N-methyl-phenanthrolinium (DMP) cation in solutions containing DNA are strongly affected by the addition of the paramagnetic manganese (II) ions due to the electron-nuclear dipolar interaction in the ternary Mn-DNA-DMP complex. Two possible models for the DMP-DNA intercalation complex are examined and one of them is unequivocally discriminated on the basis of the proton relaxation data. It is concluded that in the intercalation complex the long axis of the DMP molecule is almost perpendicular to the hydrogen bonds of the DNA base-pairs.     

Structure of the complex between lac repressor headpiece and operator DNA from measurements of the orientation relaxation and the electric dichroism.

The complex between lac repressor headpiece and short rodlike DNA fragments containing the lac operator sequence is characterised by measurements of the rotation diffusion. Using the method of electric dichroism we measure the rotation relaxation and determine changes in the length of the DNA upon ligand binding with high accuracy. According to these measurements any change in the length of the operator DNA upon binding of the first two headpiece molecules remains below 1A; the electric dichroism also remains virtually unchanged. At high degrees of (unspecific) binding we observe an increase in the rotation relaxation time, which is attributed to an increase of the apparent mean radius of the complex. As a control of our procedure for the determination of length changes we use the intercalation of ethidium bromide and arrive at an increase of the DNA length per bound ethidium of 3.2A (at 3.4A rise per base pair). The results obtained for the headpiece operator complex are not consistent with models assuming large changes of the DNA structure or intercalation of tyrosine residues.     

Sodium-23 NMR spin-lattice relaxation rate studies of mono- and bis-intercalation in DNA

23Na spin-lattice relaxation rate (1/T1 = R1) measurements have been used to study the intercalation of a series of 9-aminoacridine derivatives in DNA. The 23Na relaxation rate is strongly dependent upon the amount of intercalator added to a sodium DNA solution. The results are analyzed by a combined use of the ion condensation theory and the quadrupolar relaxation theory of polyelectrolyte solutions. This interpretation shows that the major effect in lowering the relaxation rate by intercalation is not due to the release of sodium ions but is caused by a substantial decrease in the relaxation rate Rb for the remaining bound sodium ions. Likewise, titration of NaDNA solutions with MgCl2 shows that condensation of Mg2+ on the DNA double helix reduces Rb. A good agreement between experiment and theory is found if the average lengthening following intercalation of a 9-aminoacridine moiety is assumed to be approximately 2.7 A. The distinction between mono- and bis-intercalation is clearly indicated by the results. The two bis-intercalating drugs examined are found to bis-intercalate only up to r less than or equal to 0.02. For r greater than 0.02 the drugs apparently mono-intercalate.     

Sodium-23 and lithium-7 NMR spin-lattice relaxation measurements in the study intercalation in DNA.

Sodium-23 spin-lattice relaxation rate (the reciprocal relaxation time) measurements have been used to study the intercalation of 9-aminoacridine in calf thymus DNA. The results are analyzed by a two state model based on the counterion condensation theory and a theory for the quadrupolar relaxation of counterions in polyelectrolyte solutions. It is shown that change of the solvent from H2O to D2O has a negligible effect on the intercalation process. Furthermore, an attempt is made to analyze the dependence of the 7Li spin-lattice relation rate on intercalation of 9-aminoacridine in LiDNA. It is shown that both quadrupolar and dipolar mechanisms contribute to the bound 7Li relation rate, and that both these contributions are reduced upon intercalation of 9-aminoacridine.     

Dynamics of drug-DNA interactions: a comparative temperature jump study of ellipticinium and 9-hydroxy ellipticinium

The temperature-jump method has been used to compare the binding of 2-N methyl ellipticinium (NME) and 2-N methyl 9 hydroxy ellipticinium (NMHE) to three natural DNA's of different AT/GC composition. The relaxation signals, analyzed by the Padé-Laplace method, are characterized by two distinct relaxation times, tau 1 and tau 2, respectively in the 1-4 ms and 20-80 ms range. In the case of the NMHE/DNA interaction, the slower relaxation time tau 2 depends on the DNA composition, as follows: tau 2 (Micrococcus lysodeikticus) greater than tau 2 (Calf thymus) greater than tau 2 (Clostridium perfringens). Contrary to NMHE, NME which does not possess an OH group at the C-9 position, shows no relaxation time dependence upon DNA base composition. The observation of two relaxation times indicates that the binding equilibria are associated with at least two distinct drug/DNA complexes (probably arising from two distinct DNA binding sites). Three kinetic models, involving the formation of a weak intermediate ionic complex, are given to explain the binding reaction between these cationic drugs and the DNA. They allow the determination of the four rate constants associated with the two binding steps and lead to equilibrium association constants in agreement with those obtained from spectroscopic studies. The validity of the models is discussed and it is shown that the best kinetic scheme, for either NMHE or NME, could be that in which the ionic step is not a prerequiste to intercalation. The kinetic results show that the residence time of 9 hydroxy ellipticinium is markedly increased in GC rich DNA's and this could be related to the higher in vitro and in vivo cytotoxic properties of 9 hydroxy substituted ellipticines.     

Binding of ligands to a one-dimensional heterogeneous lattice. III. Kinetic model and relaxation study of the interaction of tilorone with DNA and polynucleotides

A temperature-jump relaxation study of the interaction of tilorone with different polynucleotides and DNA has been performed. A single relaxation time, attributed to the intercalation step, has been observed in the case of poly[d(A-T)]·poly[d(A-T)], poly[d(A-C)]·poly[d(G-T)], poly[d(G-C)]·poly[d(G-C)], and poly(dG)·poly(dC). No intercalation into poly(dA)·poly(dT) occurs, and the interaction with poly(dG)·poly(dC) is different from what is observed with the other intercalating homopolymers. Refinement of the binding model is suggested from the analysis of the kinetic data. The relaxation curves obtained with DNA are well simulated based on a binding mechanism where DNA is considered a heterogeneous lattice and each type of site behaves as if it were located in the corresponding homopolymer. Poly(dA)·poly(dT) shows a unique behavior: studies of the effects of concentration and temperature indicate that tilorone acts as a probe of a process involving the polynucleotide alone. This process appears to be related to the dynamic structure of the nucleic acid and is detectable only when the bound dye is not intercalated.     

Luminescence of a Pt(II) complex in the presence of DNA. Dependence of luminescence changes on the interaction binding mode.

Luminescence intensity changes of a Pt(II) complex which is known to bind externally to DNA at low [DNA]/[complex] ratio and to intercalate at high [DNA]/[complex] ratio are studied in the presence of calf thymus DNA. External binding is demonstrated to induce luminescence enhancement whereas intercalation leads to luminescence quenching. The reasons for this behaviour are discussed.     

Restrained torsional dynamics of nuclear DNA in living proliferative mammalian cells

Physical parameters, describing the state of chromatinized DNA in living mammalian cells, were revealed by in situ fluorescence dynamic properties of ethidium in its free and intercalated states. The lifetimes and anisotropy decays of this cationic chromophore were measured within the nuclear domain, by using the ultra-sensitive time-correlated single-photon counting technique, confocal microscopy, and ultra-low probe concentrations. We found that, in living cells: 1) free ethidium molecules equilibrate between extracellular milieu and nucleus, demonstrating that the cation is naturally transported into the nucleus; 2) the intercalation of ethidium into chromatinized DNA is strongly inhibited, with relaxation of the inhibition after mild (digitonin) cell treatment; 3) intercalation sites are likely to be located in chromatin DNA; and 4) the fluorescence anisotropy relaxation of intercalated molecules is very slow. The combination of fluorescence kinetic and fluorescence anisotropy dynamics indicates that the torsional dynamics of nuclear DNA is highly restrained in living cells.     

The Interaction Between the Novel Intercalator Diethidium Cation and B-Form DNA: a Theoretical Study

Abstract

This research is an effort to further understand the physicochemical interaction between the novel drug molecule diethidium (2,7-diamino 9-[2,7 diamino 10-nN- phenanthridium] 10- nN- phenanthridium) and its biological receptor DNA. The ultimate goal is the elucidation of this novel class of drugs as potential pharmaceutical agents. Understanding the physico- chemical properties of this drug as well as the mechanism by which it interacts with DNA should ultimately allow the rational design of novel anti-cancer or anti-viral drugs.

A novel binding structure for the diethidium cation to B-form DNA is herein described. Molecular modeling on the complex formed between diethidium and a dodecamer of double-stranded B-form DNA, CGCGAATTCGCG, has shown that this complex is indeed fully capable of participating in the formation of a stable intercalation site. It was expected that diethidium would have a mechanism of intercalation significantly different from other classical intercalators because a) Its structure, that of two perpendicular planes, each known to have excellent intercalation properties, is novel b) The linker region length is zero c) The tilt between the two planes of the drug matches the geometry of the space available to this drug in the major groove.

We have studied the complex formed when diethidium enters the central site of the B-DNA dodecamer through the major groove. The complex forms several classes of intercalation structures, which are all stable and vary from “partially intercalate” to “fully intercalated”. Multiple minimizations show the drug to be very mobile within the intercalation site. Further, some structures show organization and concomitant stiffening of the DNA above the intercalation site, with a disorganization and disruption of the regular B-DNA structure immediately below the intercalation site. This particular phenomena may be expected to lead to significantly different physicochemical properties for the diethidium complex with respect to other known intercalators, because this sort of vectorial difference in structure above and below the site of intercalation is unknown in existing intercalators, as far as the authors are aware. In addition, we expect the mechanism of interaction between drug and DNA to be described by “direct ligand transfer”, wherein the drug is transferred from duplex DNA to duplex DNA without re-entering the solvent.¹

This work is the first instance known to the authors of a novel drug entity that was deduced solely by mathematical reasoning ² and described subsequently by computational methods. Evidence that diethidium should interact with its target site DNA differently from other known intercalators is strong.     

Proflavin binding to poly[d(A-T)] and poly[d(A-br5U)]: triplet state and temperature-jump kinetics

The delayed fluorescence properties of proflavin have been exploited in studies of the excited-state binding kinetics of the dye to poly[d(A-T)] and its brominated analogue poly[d(A-br5U)] at room temperature and pH 7. The two analyzed luminescence decay times of the DNA-dye complex are dependent on the total nucleic acid concentration. This dependence is shown to reflect a temporal coupling of the intrinsic delayed emission decay rates with the dynamic chemical kinetic binding processes in the excited state. Temperature-jump kinetic studies conducted on the brominated polymer and corresponding information on poly[d(A-T)] from a previous study [Ramstein, J., Ehrenberg, M., & Rigler, R. (1980) Biochemistry 19, 3938-3948] provide complementary information about the ground state. In the ground state, the poly[d(A-T)]-proflavin complex has one chemical relaxation time, which reaches a plateau at high DNA concentrations. The brominated DNA-dye complex exhibits two relaxation times: a faster relaxation mode that behaves similarly to that for the unhalogenated DNA and a slower relaxation mode that is apparent at high DNA concentrations. The ground-state kinetic data are analyzed in terms of two alternative models incorporating series and parallel reaction schemes. The former consists of two sequential binding steps--a fast bimolecular process followed by a monomolecular step--while the latter consists of two coupled bimolecular steps. A similar analysis for the excited-state data yields reasonable kinetic constants only for the series model, which, in accordance with previous proposals for acridine intercalators, consists of a fast outside binding step followed by intercalation of the dye. A comparison of the ground- and excited-state kinetic parameters reveals that the external binding process is much stronger and the intercalation is much weaker in the excited state. That the excited-state data are only consistent with the series model suggests that delayed luminescence studies may provide a general tool for distinguishing between the two kinetic mechanisms. In particular, we demonstrate the use of delayed luminescence spectroscopy as a tool for probing dynamic DNA-ligand interactions in solution.     

The importance of intercalation in the covalent binding of benzo(a)pyrene diol epoxide to DNA

The primary mode of non-covalent interaction of the strong carcinogen, benzo(a)pyrene diol epoxide, with DNA is through intercalation. It has variously been suggested that intercalative complexes may be prerequisite for either covalent binding or DNA-catalysed hydrolysis of the epoxide or both. Geacintov [Geacintov, N. E. (1986). Carcinogenesis 7, 589.] has recently argued that intercalation is important in covalent binding and presented theoretical constructs consistent with this proposal. A more general theoretical model is presented here which includes the possibilities that either catalysis of hydrolysis or covalent binding of benzo(a)pyrene diol epoxide DNA can occur (a) in an intercalation complex, or (b) without formation of a detectable, physically bound complex. It is shown that a variety of possible mechanisms formulated under this general theory lead to equations for overall reaction rates and covalent binding fractions which are all of the same form with respect to DNA concentration dependence. A consequence of this is that experimental studies of the dependence of hydrolysis rates and covalent binding fractions on DNA concentration do not distinguish between the various possible mechanisms. These findings are discussed in relation to the interactions of benzo(a)pyrene diol epoxide with chromatin in cells.     

DAPI (4',6-diamidino-2-phenylindole) binds differently to DNA and RNA: minor-groove binding at AT sites and intercalation at AU sites.

The interaction of DAPI and propidium with RNA (polyA.polyU) and corresponding DNA (polydA.polydT) sequences has been compared by spectroscopic, kinetic, viscometric, Tm, and molecular modeling methods. Spectral changes of propidium are similar on binding to the AT and AU sequences but are significantly different for binding of DAPI. Spectral changes for DAPI with the DNA sequence are consistent with the expected groove-binding mode. All spectral changes for complexes of propidium with RNA and DNA and for DAPI with RNA, however, are consistent with an intercalation binding mode. When complexed with RNA, for example, DAPI aromatic protons signals shift significantly upfield, and the DAPI UV-visible spectrum shows significantly larger changes than when complexed with DNA. Slopes of log kd (dissociation rate constants) versus-log [Na+] plots are similar for complexes of propidium with RNA and DNA and for the DAPI-RNA complex and are in the range expected for an intercalation complex. The slope for the DAPI-DNA complex, however, is much larger and is in the range expected for a groove-binding complex. Association kinetics results also support an intercalation binding mode for the DAPI-RNA complex. The viscosity of polyA.polyU solutions increases significantly on addition of both propidium and DAPI, again in agreement with an intercalation binding mode for both molecules with RNA. Molecular modeling studies completely support the experimental findings and indicate that DAPI forms a very favorable intercalation complex with RNA. DAPI also forms a very stable complex in the minor groove of AT sequences of DNA, but the stabilizing interactions are considerably reduced in the wide, shallow minor groove of RNA. Modeling studies,thus,indicate that DAPI interaction energetics are more favorable for minor-groove binding in AT sequences but are more favorable for interaction in RNA.     

Ru(phen)2DPPZ]2+ is in contact with DNA bases when it forms a luminescent complex with single-stranded oligonucleotides

The luminescence intensity of the Delta- and Lambda-enantiomer of [Ru(phen)2DPPZ]2+ ([Ru(phenanthroline)2 dipyrido[3,2-a:2',3'-c]phenazine]2+) complex enhanced upon binding to double stranded DNA, which has been known as "light switch effect". The enhancement of the luminescence required the intercalation of the large ligand between DNA base pairs. In this study, we report the enhancement in the luminescence intensity when the metal complexes bind to single stranded oligonucleotides, indicating that the "light switch effect" does not require intercalation of the large DPPZ ligand. Oligonucleotides may provide a hydrophobic cavity for the [Ru(phen)2DPPZ]2+ complex to prevent the quenching by the water molecule. In the cavity, the metal complex is in contact with DNA bases as is evidenced by the observation that the excited energy of the DNA bases transfer to the bound metal complex. However, the contact of the metal complex with DNA bases is different from the stacking of DPPZ in the intercalation pocket. In addition to the normal two luminescence lifetimes, a short lifetime in the range of 1-2 ns was found for both the delta- and lambda-enantiomer of [Ru(phen)2DPPZ]2+ when complexed with single stranded oligonucleotides, which may be assigned to the metal complex that is outside of the cavity, interacting with phosphate groups of DNA.     

Copper-activated DNA photocleavage by a pyridine-linked bis-acridine intercalator

We report the synthesis of new photonuclease 4 consisting of two acridine rings joined by a pyridine-based copper binding linker. We have shown that photocleavage of plasmid DNA is markedly enhanced when this ligand is irradiated in the presence of copper(II) (419 nm, 22 degrees C, pH 7.0). Viscometric data indicate that 4 binds to DNA by monofunctional intercalation, and equilibrium dialysis provides an estimated binding constant of 1.13 x 105 M-1 for its association with calf thymus DNA. In competition dialysis experiments, 4 exhibits preferential binding to GC-rich DNA sequences. When Cu(II) is added at a ligand to metal ratio of 1:1, electrospray ionization mass spectrometry demonstrates that compound 4 undergoes complex formation, while thermal melting studies show a 10 degrees C increase in the Tm of calf thymus DNA. Groove binding and intercalation are suggested by viscometric data. Finally, colorimetric and scavenger experiments indicate that the generation of Cu(I), H2O2, and superoxide contributes to the production of DNA frank strand breaks by the Cu(II) complex of 4. Whereas the strand breaks are distributed in a relatively uniform fashion over the four DNA bases, subsequent piperidine treatment of the photolysis reactions shows that alkaline labile lesions occur predominantly at guanine.     

Crystal structure of the 2:1 complex between d(GAAGCTTC) and the anticancer drug actinomycin D.

The crystal structures of the 2:1 complex of the self-complementary DNA octamer d(GAAGCTTC) with actinomycin D has been determined at 3.0 A resolution. This is the first example of a crystal structure of a DNA-drug complex in which the drug intercalates into the middle of a relatively long DNA segment. The results finally confirmed the DNA-actinomycin intercalation model proposed by Sobell & co-workers in 1971. The DNA molecule adopts a severely distorted and slightly kinked B-DNA-like structure with an actinomycin D molecule intercalated in the middle sequence, GC. The two cyclic depsipeptides, which differ from each other in overall conformation, lie in the minor groove. The complex is further stabilized by forming base-peptide and chromophore-backbone hydrogen bonds. The DNA helix appears to be unwound by rotating one of the base-pairs at the intercalation site. This single base-pair unwinding motion generates a unique asymmetrically wound helix at the binding site of the drug, i.e. the helix is loosened at one end of the intercalation site and tightened at the other end. The large unwinding of the DNA by the drug intercalation is absorbed mostly in a few residues adjacent to the intercalation site. The asymmetrical twist of the DNA helix, the overall conformation of the two cyclic depsipeptides and their interaction mode with DNA are correlated to each other and rationally explained.     

Aryl substituted ruthenium bis-terpyridine complexes: intercalation and groove binding with DNA

The non-covalent interaction of five novel ruthenium(II) bis-terpyridine complexes with calf thymus DNA and, where appropriate, with poly[d(G-C)](2) and poly[d(A-T)](2) is described. Each complex is functionalised with aryl tail groups in the 4' position of the terpyridine ligands ((i) 9-anthracenyl, (ii) 4,4'-biphenyl, (iii) beta-naphthyl, (iv) 9-phenanthrenyl, and (v) 1-pyrenyl). Circular dichroism and linear dichroism show that the binding of three of the complexes (phenanthrenyl, anthracenyl and pyrenyl) at low metal complex concentration is dominated by intercalation of the aryl tail groups between the DNA bases. The complex with the biphenyl tail predominantly exhibits groove binding with no significant tail intercalation. The naphthyl derivative binds both by intercalation and a non-intercalative mode even at low metal complex concentrations. At high metal complex concentrations, aggregation of the complexes on the DNA is observed. Resonance light scattering indicates that the aggregates are of low nuclearity along the groove.     

Viscosity dependence of ethidium-DNA intercalation kinetics

The kinetics of ethidium intercalation into double-stranded poly[d(G-C)] were investigated by use of repetitive pressure-jump chemical relaxation at 20 degrees C in low ionic strength (0.1 M NaCl) aqueous buffers containing either glycerol or methanol. The viscosity of the various solvents differed by more than an order of magnitude while other physical properties (e.g., dielectric constant) remained approximately constant. The single-reciprocal kinetic relaxation time (tau -1) increases linearly with DNA concentration. The observed association rate constant is lower in all organic-aqueous mixtures than in water and is inversely proportional to the viscosity. These results provide evidence for an additional step in the intercalation mechanism which is identified as an obligatory DNA conformational change preceding ethidium intercalation. From the data presented, the equilibrium constant of this local conformational change is approximately 10(-3), i.e., greatly favoring the structure incapable of intercalation. The corresponding kinetics were not directly determined; however, in order to be consistent with all of the data the forward and/or reverse rate constants of the conformational change must be larger than the rate of the intercalation reaction. Thus, it is proposed that the rate of the conformational change back to the nonintercalating B-DNA structure is greater than approximately 500 s-1, implying a rate of opening greater than approximately 0.5 s-1, in agreement with other hydrogen exchange and NMR data. The observed overall rate constant for the dissociation of ethidium is inversely proportional to the solvent density, possibly reflecting a dependence on the solvent free volume. The overall volume change of intercalation is less negative in the organic-aqueous solvent mixtures than in water.     

The intercalation of imidazoacridinones into DNA induces conformational changes in their side chain

Imidazoacridinones (IAs) are a new group of highly active antitumor compounds. The intercalation of the IA molecule into DNA is the preliminary step in the mode of action of these compounds. There are no experimental data about the structure of an intercalation complex formed by imidazoacridinones. Therefore the design of new potentially better compounds of this group should employ the molecular modelling techniques. The results of molecular dynamics simulations performed for four IA analogues are presented. Each of the compounds was studied in two systems: i) in water, and ii) in the intercalation complex with dodecamer duplex d(GCGCGCGCGCGC)2. Significant differences in the conformation of the side chain in the two environments were observed for all studied IAs. These changes were induced by electrostatic as well as van der Waals interactions between the intercalator and DNA. Moreover, the results showed that the geometry of the intercalation complex depends on: i) the chemical constitution of the side chain, and ii) the substituent in position 8 of the ring system.