Dynamics of vibrational frequency fluctuations in deuterated liquid ammonia: roles of fluctuating hydrogen bonds and free ND modes

We present an ab initio molecular dynamics study of the roles of fluctuating hydrogen bonds and free ND modes in the dynamics of ND stretch frequency fluctuations in deuterated liquid ammonia. We have also looked at some of the other dynamical quantities such as diffusion and orientational relaxation and also structural quantities such as pair correlations and hydrogen bonding properties which are relevant in the current context. The time correlation function of ND stretch frequencies is found to decay with primarily two time scales: A short-time decay with a time scale of less than 100 fs arising from intermolecular motion of intact hydrogen bonds and also from fast hydrogen bond breaking and a longer time scale of about 500 fs which can be assigned to the lifetime of free ND modes. Unlike water, in liquid ammonia an ND mode is found to remain free for a longer period than it stays hydrogen bonded and this longer lifetime of free ND modes determines the long-time behaviour of frequency fluctuations. Our hole dynamics calculations produced results of vibrational spectral diffusion that are similar to the decay of frequency time correlation. Inclusion of dispersion corrections is found to make the dynamics slightly faster.     

Two Binding Modes of Netropsin are Involved in the Complex Formation with Poly(dA-dT)·Poly(dA-dT) and other Alternating DNA Duplex Polymers

Abstract

Using CD measurements we show that the interaction of netropsin to poly(dA-dT)·poly(dA-dT) involves two binding modes at low ionic strength. The first and second binding modes are distinguished by a defined shift of the CD maximum and the presence of characteristic isodichroic points in the long wavelength range from 313 nm to 325 nm. The first binding mode is independent of ionic strength and is primarily determined by specific interaction to dA·dT base pairs. Employing a netropsin derivative and different salt conditions it is demonstrated that ionic contacts are essential for the second binding mode. Other alternating duplexes and natural DNA also exhibit more or less a second step in the interaction with netropsin observable at high ratio of ligand per nucleotide. The second binding mode is absent for poly(dA)·poly(dT). The presence of a two-step binding mechanism is also demonstrated in the complex formation of poly(dA-dT)·poly(dA-dT) with the distamycin analog consisting of pentamethylpyrrolecarboxamide. While the binding mode I of netropsin is identical with its localization in the minor groove, for binding mode II we consider two alternative interpretations.     

Two binding modes of netropsin are involved in the complex formation with poly(dA-dT).poly(dA-dT) and other alternating DNA duplex polymers

Using CD measurements we show that the interaction of netropsin to poly(dA-dT).poly(dA-dT) involves two binding modes at low ionic strength. The first and second binding modes are distinguished by a defined shift of the CD maximum and the presence of characteristic isodichroic points in the long wavelength range from 313 nm to 325 nm. The first binding mode is independent of ionic strength and is primarily determined by specific interaction to dA.dT base pairs. Employing a netropsin derivative and different salt conditions it is demonstrated that ionic contacts are essential for the second binding mode. Other alternating duplexes and natural DNA also exhibit more or less a second step in the interaction with netropsin observable at high ratio of ligand per nucleotide. The second binding mode is absent for poly(dA).poly(dT). The presence of a two-step binding mechanism is also demonstrated in the complex formation of poly(dA-dT).poly(dA-dT) with the distamycin analog consisting of pentamethylpyrrolecarboxamide. While the binding mode I of netropsin is identical with its localization in the minor groove, for binding mode II we consider two alternative interpretations.     

Structure and Dynamics of Netropsin-Poly(dA-dT)· Poly(dA-dT) Complex: 500 MHz 1H NMR Studies

Abstract

Antibiotic netropsin is known to bind specifically to A and T regions in DNA; the mode of binding being non-intercalative. Obviously, H-bonding between the proton donors of netropsin and acceptors N3 of A and 02 of T comes as a strong possibility which might render this specificity. In netropsin there could be 8 proton donors: four terminal amino groups and four internal imino groups. However, methylation of the terminal amino groups does not alter the binding affinity of netropsin to DNA—but the modification of the internal imino groups significantly lowers the binding affinity. Hence, the logical conclusion is that netropsin may specifically interact with A and T through H-bonding and in order to do so, it should approach the helix from the minor groove. The present paper provides experimental data which verify the conclusion mentioned above.

Using poly(dA-dT)? poly(dA-dT) as a model system it was observed following a thorough theoretical stereochemical analysis that netropsin could bind to -(T-A-T) sequence of the polymer in the B-form through the minor groove by forming specific B-bonding. Models could be either right or left-handed B-DNA with a mono or dinucleotide repeat.

By monitoring the ³¹P signals of free poly(dA-dT) ? poly(dA-dT) and netropsin-poly(dA-dT)? poly(dA-dT) complex we show that the drug changes the DNA structure from essentially a mononucleotide repeat to that of very dominant dinucleotide repeat; however the base- pairing in the DNA-drug complex remain to be Watson-Crick. Whether H-bonding is the specific mode of interaction was judged by monitoring the imino protons of netropsin in the presence of poly(dA-dT) ? poly(dA-dT). This experiment was conducted in 90% H₂O + 10% D₂O Using the time-shared long pulse. It was found that exchangeable imino protons of netropsin appear in the drug-DNA complex and disappear upon increasing the D₂O content; thus confirming that H-bonding is indeed the specific mode of interaction. From these and several NOE measurements, we propose a structure for poly(dA-dT)? poly(dA-dT(-netropsin complex.

In summary, experimental data indicate that netropsin binds to poly(dA-dT)? poly(dA-dT) by forming specific hydrogen bonds and that the binding interaction causes the structure to adopt a Watson-Crick paired dinucleotide repeat motif. The proposed hydrogen bonds can form only if the drug approaches the DNA from the minor groove. Within the NMR time scale the interaction between the ligand and DNA is a fast one. From the NOE experimental data, it appears that poly(dA-dT)? poly(dA-dT) in presence of netropsin exists as an equilibrium mixture of right- and left-handed B-DNA duplexes with a dinucleotide repeat—with a predominance of the left-handed form. The last conclusion is a soft one because it was very difficult to make sure the absence of spin diffusion. In a 400 base pairs long DNA duplex- drug complex (as used in this study), equilibrium between right and left-handed helices can also mean the existence of both helical domains in the same molecule with fast interchange between these domains or/and unhindered motion/propagation of these domains along the helix axis.     

Influence of Drug Binding on DNA Flexibility: A Normal Mode Analysis

Abstract

DNA-drug complexes are important because of their pharmacological interest but, in addition, they provide a useful model to study the essential aspects of DNA recognition processes. In order to investigate the influence of ligand binding on the dynamic properties of DNA we have carried out normal mode analysis for complexes with drugs of two types: a typical intercalator, 9-aminoacridine, and a typical groove binder, netropsin. Normal modes are analysed in terms of helicoidal parameter variations with special attention being paid to global deformations of the double helix. The results show that the influence of these two drugs is very different. Intercalation of 9-aminoacridine leads to an increase in the flexibility of the intercalated dinucleotide step, with notably larger vibrational amplitudes for both roll and twist parameters compared to free DNA. In contrast, the groove binding of netropsin induces a stiffening of the DNA segment which is in contact with the drug reflected by decreased vibrational amplitudes for backbone angles and inter base pair helicoidal parameters and an increase in vibrations for adjacent base pairs in terms of buckle and propeller twist.     

Molecular structure of the netropsin-d(CGCGATATCGCG) complex: DNA conformation in an alternating AT segment

The molecular structure of the complex between a minor groove binding drug (netropsin) and the DNA dodecamer d(CGCGATATCGCG) has been solved and refined by single-crystal X-ray diffraction analysis to a final R factor of 20.0% to 2.4-A resolution. The crystal is similar to that of the other related dodecamers with unit cell dimensions of a = 25.48 A, b = 41.26 A, and c = 66.88 A in the space group P2(1)2(1)2(1). In the complex, netropsin binds to the central ATAT tetranucleotide segment in the narrow minor groove of the dodecamer B-DNA double helix as expected. However, in the structural refinement the drug is found to fit the electron density in two orientations equally well, suggesting the disordered model. This agrees with the results from solution studies (chemical footprinting and NMR) of the interactions between minor groove binding drugs (e.g., netropsin and distamycin A) and DNA. The stabilizing forces between drug and DNA are provided by a combination of ionic, van der Waals, and hydrogen-bonding interactions. No bifurcated hydrogen bond is found between netropsin and DNA in this complex due to the unique dispositions of the hydrogen-bond acceptors (N3 of adenine and O2 of thymine) on the floor of the DNA minor groove. Two of the four AT base pairs in the ATAT stretch have low propeller twist angles, even though the DNA has a narrow minor groove. Alternating helical twist angles are observed in the ATAT stretch with lower twist in the ApT steps than in the TpA step.     

Low-frequency dynamics and Raman scattering of crystals, of B-, A-, and Z-DNA, and fibers of C-DNA

Normal modes of vibration of DNA in the low-frequency region (10-300 cm-1 interval) have been identified from Raman spectra of crystals of B-DNA [d(CGCAAATTTGCG)], A-DNA [r(GCG)d(CGC) and d(CCCCGGGG)], and Z-DNA [d(CGCGCG) and d(CGCGTG)]. The lowest vibrational frequencies detected in the canonical DNA structures--at 18 +/- 2 cm-1 in the B-DNA crystal, near 24 +/- 2 cm-1 in A-DNA crystals, and near 30 +/- 2 cm-1 in Z-DNA crystals--are shown to correlate well with the degree of DNA hydration in the crystal structures, as well as with the level of hydration in calf thymus DNA fibers. These findings support the assignment [H. Urabe et al. (1985) J. Chem. Phys. 82, 531-535; C. Demarco et al. (1985) Biopolymers 24, 2035-2040] of the lowest frequency Raman band of each DNA to a helix mode, which is dependent primarily upon the degree of helix hydration, rather than upon the intrahelical conformation. The present results show also that B-, A-, C-, and Z-DNA structures can be distinguished from one another on the basis of their characteristic Raman intensity profiles in the region of 40-140 cm-1, even though all structures display two rather similar and complex bands centered within the intervals of 66-72 and 90-120 cm-1. The similarity of Raman frequencies for B-, A-, C-, and Z-DNA suggests that these modes originate from concerted motions of the bases (librations), which are not strongly dependent upon helix backbone geometry or handedness. Correlation of the Raman frequencies and intensities with the DNA base compositions suggests that the complex band near 90-120 cm-1 in all double-helix structures is due to in-plane librational motions of the bases, which involve stretching of the purine-pyrimidine hydrogen bonds. This would explain the centering of the band at higher frequencies in structures containing G.C pairs (greater than 100 cm-1) than in structures containing A.T pairs (less than 100 cm-1), consistent with the strengths of G.C and A.T hydrogen bonding.     

Binding of an antitumor drug to DNA, Netropsin and C-G-C-G-A-A-T-T-BrC-G-C-G

The antitumor antibiotic netropsin has been co-crystallized with a double-helical B-DNA dodecanucleotide of sequence: C-G-C-G-A-A-T-T-BrC-G-C-G, and the structure of the complex has been solved by X-ray diffraction at a resolution of 2.2 A. The structure has been refined independently by Jack-Levitt and Hendrickson-Konnert least-squares methods, leading to a final residual error of 0.257 by the Jack-Levitt approach (0.211 for two-sigma data) or 0.248 by the Hendrickson-Konnert approach, with no significant difference between refined structures. The netropsin molecule displaces the spine of hydration and fits snugly within the minor groove in the A-A-T-T center. It widens the groove slightly and bends the helix axis back by 8 degrees, but neither unwinds nor elongates the double helix. The drug molecule is held in place by amide NH hydrogen bonds that bridge adenine N-3 and thymine O-2 atoms, exactly as with the spine of hydration. The requirement of A X T base-pairs in the binding site arises because the N-2 amino group of guanine would demand impermissibly close contacts with netropsin. It is proposed that substitution of imidazole for pyrrole in netropsin should create a family of "lexitropsins" capable of reading G X C-containing base sequences.     

Binding of netropsin to a DNA triple helix.

The interaction of netropsin, a minor groove binding drug, with T-A-T triple helix and A-T double helix was studied using circular dichroism spectroscopy and thermal denaturation. The triple helix was made by an oligonucleotide (dA)12-x-(dT)12-x-(dT)12, where x is a hexaethylene glycol chain bridged between the 3' phosphate of one strand and the 5' phosphate of the following strand. This oligonucleotide is able to fold back on itself to form a very stable triplex. Changing the conditions allows the same oligonucleotide in a duplex form with a (dT)12 dangling arm. Circular dichroism spectroscopy demonstrates that netropsin can bind to the triple helical structure. Spectral analysis shows that the bound drug exhibits a conformation and an environment similar in double-stranded and in triple-stranded structure. However, the binding constant to the triple-stranded structure is found smaller than the binding constant to the double-stranded one. Thermal denaturation experiments demonstrate that netropsin destabilizes the triplex whereas it stabilizes the duplex.     

Quantitative footprinting analysis using a DNA-cleaving metalloporphyrin complex

The results of quantitative footprinting studies involving the antiviral agent netropsin and a DNA-cleaving cationic metalloporphyrin complex are presented. An analysis of the footprinting autoradiographic spot intensities using a model previously applied to footprinting studies involving the enzyme DNase I [Ward, B., Rehfuss, R., Goodisman, J., & Dabrowiak, J. C. (1988) Biochemistry 27, 1198-1205] led to very low values for netropsin binding constants on a restriction fragment from pBR-322 DNA. In this work, we show that, because the porphyrin binds with high specificity to DNA, it does not report site loading information in the same manner as does DNase I. We elucidate a model involving binding equilibria for individual sites and include competitive binding of drug and porphyrin for the same site. The free porphyrin and free drug concentrations are determined by binding equilibria with the carrier (calf thymus DNA) which is present in excess and acts as a buffer for both. Given free porphyrin and free netropsin concentrations for each total drug concentration in a series of footprinting experiments, one can calculate autoradiographic spot intensities in terms of the binding constants of netropsin to the various sites on the 139 base pair restriction fragment. The best values of these binding constants are determined by minimizing the sum of the squared differences between calculated and experimental footprinting autoradiographic spot intensities. Although the determined netropsin binding constants are insensitive to the value assumed for the porphyrin binding constant toward its highest affinity sites, the best mean-square deviation between observed and calculated values, D, depends on the choice of (average) drug binding constant to carrier DNA, Kd.(ABSTRACT TRUNCATED AT 250 WORDS)     

Netropsin Specifically Recognizes One of the Two Conformationally Equivalent Strands of Poly (dA)·Poly (dT). One Dimensional NMR Study at 500 MHz Involving NOE Transfer Between Netropsin and DNA Protons

Abstract

Recent observations that the heteronomous structural model for poly(dA)·poly(dT) is not found in solution and that in this DNA, the two strands are conformationally equivalent (J. Biomole. Str. Dyns. 2, 1057 (1985)), has added a new dimension to the structural dynamics of DNA-netropsin complex. Does the antibiotic somehow distinguish between the two strands and specifically interact with only one of the conformationally equivalent strands?

Model-building studies suggest that netropsin can either bind to the dA-strand in the minor groove such that H-bonds are formed between the imino protons N4-H, N6-H, N8-H of netropsin and N3 atoms of A or can bind to the dT-strand in the minor groove and form H-bonds between the imino-protons N4-H, N6-H, N8-H of netropsin and O2 atoms of T. If netropsin binds to the dA-strand, AH2 atoms of poly(dA)-poly(dT) would be in closer proximity to the imino protrons N4-H, N6-H, N8-H and pyrrole ring protons C5-H, Cll-H of netropsin than they would be, if netropsin binds to the dT-strand. In order to distinguish these possibilities experiments were conducted which involved NOE energy transfer between netropsin and DNA protons in the drug-DNA complex. Difference NOE spectra of netropsin·poly(dA)-poly(dT) complex in which AH2 was irradiated indicate that dominant NOEs were observed at the imino and pyrrole ring protons of netropsin. When the netropsin pyrrole ring protons were irradiated, the magnetization transfer was at AH2 of DNA. These observations suggest that netropsin binds to the dA-strand of poly(dA)-poly(dT) even though dA/dT strands are conformationally equivalent.     

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.     

Experimental studies on the nature of bonding of DNA*bipyridyl-(ethylenediamine)platinum(II) and DNA*netropsin complexes in solution and oriented wet-spun films

The stability of complexes of NaDNA with bipyridyl- (ethylenediamine)platinum(II) (abbreviated [(bipy)Pt(en)](2+)) and with netropsin has been studied using two techniques: (i) ultraviolet (UV) melting experiments were done on NaDNA* [(bipy)Pt(en)](2+), showing that the [(bipy)Pt(en)](2+) ligand stabilizes the DNA double helix structure; and (ii) swelling measurements (via optical microscopy) as a function of relative humidity were done on wet-spun oriented films of NaDNA*[(bipy)Pt(en)](2+) and of NaDNA*netropsin. The swelling data shows that an irreversible transition of the films occurs at high relative humidity, first for the NaDNA*netropsin, then for pure NaDNA, and lastly for the NaDNA*[(bipy)Pt(en)](2+). These results are indicative that the [(bipy)Pt(en)](2+) complex stabilizes the intermolecular bonds which mediate the film swelling characteristics. A model is suggested for the binding of [(bipy)Pt(en)](2+) to DNA to explain why the swelling experiments show this ligand as increasing the intermolecular bond strength between the DNA double helices, while netropsin decreases this degree of stabilization.     

Conformational changes in sensory rhodopsin I: similarities and differences with bacteriorhodopsin, halorhodopsin, and rhodopsin

FTIR difference spectra have been obtained for the sR587----S373 phototransition of sensory rhodopsin I (sR-I), a signal-transducing protein of Halobacterium halobium. The vibrational modes of the sR587 chromophore have frequencies close to those of the bacteriorhodopsin bR568 chromophore, confirming that the two chromophores have very similar structures and environments. However, the sR-I Schiff base C = N stretch frequency is downshifted relative to bR, consistent with weaker hydrogen bonding with its counterion(s). The carboxyl (COOH) stretch modes of sR-I and halorhodopsin (hR) are at the same frequencies. On the basis of sequence homologies, these bands can be assigned to Asp-106 in helix D and/or Asp-201 in helix G. In contrast, no band was found that could be assigned to the protonation of Asp-76. In bR, the homologous residue Asp-85 serves as the acceptor group for the Schiff base proton. Bands appear in the amide I and II regions at similar frequencies in sR-I, hR, and bR, indicating that despite their different functions they all undergo closely related structural changes. Bands are also detected in the C-H stretch region, possibly due to alterations in the membrane lipids. Similar spectral features are also observed in the lipids of rhodopsin-containing photoreceptor membrane upon light activation.     

Sequence and temperature dependence of the interbase hydrogen-bond breathing modes in B-DNA polymers: Comparison with low-frequency Raman peaks and their role in helix melting

We carry out temperature-dependent lattice dynamics calculations to determine the vibrational normal modes associated with the interbase H-bond breathing motion in several B-DNA copolymers at temperatures from room temperature to the melting temperatures. We take into consideration Raman selection rules and incorporate a simple empirical model of Raman susceptibility in the interbase H bonds in our calculation and compare them to Raman measurements. Our calculations are carried out using empirical force constants that are not further refined to low-frequency spectra. Our calculations show the existence of strong interbase H-bond breathing modes at frequencies and with relative oscillator strengths close to the observed Raman peaks in the range of 60–140 cm^?1 for the DNA sequences considered except for one helix. The correlation between the calculated and observed frequencies and oscillator strengths indicates that the observed Raman peaks in the frequency range are likely interbase H-bond breathing modes. We find that these modes exhibit sizable temperature as well as sequence dependence. We show the softening of these modes on approaching thermal denaturation that is also in agreement with the observed behavior in Raman and melting measurements. The sensitivity of the calculation on the empirical model of Raman susceptibility and the possible reasons for the discrepancy between a few calculated values and observations are discussed. © 1995 John Wiley & Sons, Inc.     

RF absorption involving biological macromolecules

The fundamental intramolecular frequency of a globular protein can be obtained from the measurements of acoustic velocities of bulk protein matter. This lowest frequency for common size molecules is shown to be above several hundred GHz. All modes below this frequency would then be intermolecular modes or bulk modes of the molecule and surrounding matter or tissue. The lowest frequency modes of an extended DNA double helix are also shown to be bulk modes because of interaction with water. Only DNA modes, whose frequency is well above 4 GHz, can be intrahelical modes, that is, confined to the helix rather than in the helix plus surroundings. Near 4 GHz, they are heavily damped and, therefore, not able to resonantly absorb. Modes that absorb radio frequency (RF) below this frequency are bulk modes of the supporting matter. Bulk modes rapidly thermalize all absorbed energy. The implication of these findings for the possibility of athermal RF effects is considered. The applicability of these findings for other biological molecules is discussed.     

Protection of (dA.dT) cluster regions in the DNAase I cleavage of DNA by specific interaction with netropsin

The specific DNA binding ligand netropsin selectively blocks dA-dT base pairs in clusters containing two or more consecutive thymine residues at the dNAase I cleavage sites of DNA. Using CD and UV absorption measurements it is shown, that at various ratios of netropsin to nucleotide concentrations and even at satuation of ligand interaction the enzyme cuts along regions containing dG-dC pairs sandwiched between dA-dT pairs. This follows a slow kinetics and is associated with a release of netropsin from those segments. These facts suggests the usefulness of the partial protection of certain DNA sequences in DNAase I cleavage sites in producing DNA fragments in structural studies of the genome. A possible interpretation of the effect of netropsin binding on the enzymatic hydrolysis of phosphodiester bonds of the helix is discussed.     

Stability of triple-helical poly(dT)-poly(dA)-poly(dT) DNA with counterions.

Structural conformation of triple-helical poly(dT)-poly(dA)-poly(dT) has been a very controversial issue recently. Earlier investigations, based on fiber diffraction data and molecular modeling, indicated an A-form conformation with C'3-endo sugar pucker. On the other hand, Raman, solution infrared spectral, and NMR studies show a B-form structure with C'2-endo sugars. In accordance with these experimental results, a theoretical model with B-form, C'2-endo sugars was proposed in 1993. In the present work we investigate the dynamics and stability of the two conformations within the effective local field approach applied to the normal mode calculations for the system. The presence of counterions was explicitly taken into account. Stable equilibrium positions for the counterions were calculated by analyzing the normal mode dynamics and free energy of the system. The breathing modes of the triple helix are shifted to higher frequencies over those of the double helix by 4-16 cm-1. The characteristic marker band for the B conformation at 835 cm-1 is split up into two marker bands at 830 and 835 cm-1. A detailed comparison of the normal modes and the free energies indicates that the B-form structure, with C'2-endo sugar pucker, is more stable than the A-form structure. The normal modes and the corresponding dipole moments are found to be in close agreement with recent spectroscopic findings.     

Molecular Modelling Study of the Netropsin Complexation With a Nucleic Acid Triple Helix

Abstract

A detailed molecular mechanical study has been made on the complexes of netropsin with the double stranded oligonucleotide (dA)₁₂.(dT)₁₂ and with the triple helix (dA)₁₂.(dT)₁₂.(dT)₁₂. The complexes were built using computer graphics and energy refined using JUMNA program. In agreement with circular dichroïsm experiments we have shown that 3 netropsins can bind the minor grooves of the triple helix and of the double helix. The groove geometry in the duplex and in the triplex is very similar. However a detailed analysis of the energetic terms shows, in agreement with thermal denaturation studies, that the affinity of netropsin toward the double helices is larger than towards triple helices.     

Netropsin and bis-netropsin analogs as inhibitors of the catalytic activity of mammalian DNA topoisomerase II and topoisomerase cleavable complexes.

This study examined the ability of netropsin and related minor groove binders to interfere with the actions of DNA topoisomerases II and I. We evaluated a series of netropsin dimers linked with flexible aliphatic chains of different lengths. These agents are potentially able to occupy longer stretches of DNA than the parental drug as a result of bidentate binding. Both netropsin and its dimers were found: (i) to inhibit the catalytic activity of isolated topoisomerase II and (ii) to interfere with the stabilization of the cleavable complexes of topoisomerase II and I in nuclei. Dimers with linkers consisting of 0-4 and 6-9 methylene groups (n) were far more inhibitory than netropsin against isolated enzyme and in the nuclear system. The compound with n = 5 was less active than netropsin in both assays while the dimer with n = 10 inhibited only the isolated enzyme. The comparison of dimers with fixed linker length (n = 2) but varying number of N-methylpyrrole residues (from 1 to 3) revealed that the inhibitory properties were enhanced with increasing number of N-methylpyrrole units. For dimers with varying linker length, drug ability to inhibit catalytic activity of isolated topoisomerase II was positively correlated with calf thymus DNA association constants. In contrast, no such correlation existed in nuclei. However, the inhibitory effects in the nuclear system were correlated with the association constants for poly(dAdT). The results indicate that bidentate binding can significantly enhance anti-topoisomerase activity of netropsin related dimeric minor groove binders. However, other factors such as the length of the linker, the number of pyrrole moieties and the nature of the target (isolated enzyme/DNA versus chromatin in nuclei) also contribute to these activities.