X-ray diffraction and infrared circular dichroism of DNA-violamycin B1 complexes

X-ray diffraction and infrared linear dichroism of oriented samples of DNA-violamycin B1 complexes have been studied at different antibiotic/DNA phosphate ratios (r) as a function of relative humidity. Violamycin B1 binds to DNA according to the intercalation as well as to the outside binding model. At low r values, where the intercalation predominates the unwinding angle of DNA helix is between 6 degrees and 12 degrees per intercalation site as followed from the dependence of the pitch of helix versus r. At r greater than or equal to 0.17 the intercalation sites are saturated and the outside binding becomes prevalent; however the violamycin B1 chromophore is still oriented in the plane of DNA bases. Conformational mobility of DNA in the violamycin B1 complexes is largely inhibited compared with pure DNA, but it is higher than that of the daunomycin complexes. At least 30% of DNA in violamycin complexes has A conformation at the medium humidities as followed by IR linear dichroism. In the case of x-ray diffraction the A conformation was not detected. The distance between DNA molecules in the complex is found to be 23.2 A, that is 2 A less than in pure DNA at the same conditions and it does not depend upon r.     

Porphyrin and metalloporphyrin binding to DNA polymers: rate and equilibrium binding studies

Interactions of meso-tetrakis(4-N-methylpyridiniumyl)porphyrin [TMpyP(4)] with poly[d(G-C)].poly[d(G-C)] [poly[d(G-C)2] and poly[d(A-T)].poly[d(A-T)] [poly[d(A-T)2] were studied by equilibrium dialysis and stopped-flow dissociation kinetics as a function of [Na+]. Metalloderivatives of TMpyP(4), NiTMpyP(4), and ZnTMpyP(4) were also investigated. The apparent equilibrium binding constants (Kobs) were approximately the same for TMpyP(4) binding to either poly[d(G-C)2] or poly[d(A-T)2] and decreased with increasing [Na+]. The slopes of the plots of log Kobs vs log [Na+] were similar, with values close to -2.7. Contrary to implications in previously reported studies, these data do not indicate that TMpyP(4) prefers to bind to GC sites at low ionic strength and to AT sites at high ionic strength. In contrast, binding of ZnTMpyP(4) to these two polymers is very different. Comparisons of Kobs values at 0.065 M [Na+] indicate that ZnTMpyP(4) binding to AT sites is approximately 200 times more favorable than binding to GC sites, a finding in agreement with previous qualitative observations. Although the binding of the Zn species to the GC polymer was too weak for us to assess the salt effect, the plot of log Kobs vs log [Na+] gave a slope of -2.0 for ZnTMpyP(4) binding to poly[d(A-T)2]. Application of condensation theory for polyelectrolytes suggests similar charge interactions for ZnTMpyP(4) and for TMpyP(4) binding to poly[d(A-T)2]. Likewise, the rates of dissociation from poly[d(A-T)2] were similar for TMpyP(4) and ZnTMpyP(4) [and also NiTMpyP(4)]. However, whereas TMpyP(4) [and NiTMpyP(4)] dissociation from poly[d(G-C)2] was measurable, that for ZnTMpyP(4) was too fast to measure.(ABSTRACT TRUNCATED AT 250 WORDS)     

Comparison of the effects of cationic porphyrins on DNA properties: influence of GC content of native and synthetic polymers

Interactions of meso-tetra(4-N-methylpyridyl)porphyrin [TMpyP(4)], meso-tetra(2-N-methylpyridyl)porphyrin [TMpyP(2)], and meso-tetra(para-N-trimethylanilinium)porphyrin (TMAP) with several native and synthetic DNAs were studied by a variety of physical techniques: nmr (³¹P and ¹H), absorption spectroscopy, viscosity, and flow dichroism (FD). Of the three porphyrins studied, only the interaction of TMpyP(4) with poly [d(G-C)₂] was fully consistent with intercalation. In particular, a large increase in viscosity, a downfield ³¹P-nmr signal (ca. -1 ppm), and upfield imino proton signals (11 to 12 ppm range) were observed. Comparison of the effects of TMpyP(4) on DNAs of different GC contents revealed larger changes in solution viscosity with increased GC content. However, the characteristic changes in ³¹P- and ¹H-nmr spectra were not observed. The viscosity increases observed in studies with poly[d(A-C)(G-T)] and C. Perf. DNA were much lower than with poly[d(G-C)₂], M. Lys. DNA, and calf thymus DNA. Thus, GC sequence and content are clearly important. The principal change in the ³¹P-nmr signal of native DNA is the appearance of a very broad shoulder centered at ca. -2.0 ppm, which is larger in M. Lys. DNA than in C. Perf. DNA. FD studies indicate highly ordered TMpyP(4) cations arranged perpendicular to the DNA axis of calf thymus DNA. Together, these results suggest the major effects of TMpyP(4) on DNA properties are due to strong GC-binding interactions that influence DNA structure. The data are consistent with combined intercalative and outside binding interactions of TMpyP(4) with GC regions of DNA. In contrast, similar studies with TMAP suggest that it influences AT regions of DNA by an outside binding mode. On the other hand, TMpyP(2) effects on DNA properties are consistent with nonselective outside binding.     

Linear dichroism properties and orientations of different ultraviolet transition moments of benzo[a]pyrene derivatives bound noncovalently and covalently to DNA

Linear dichroism and absorption methods are used to study the orientations of transition moments of absorption bands of polycyclic aromatic epoxide derivatives which overlap with those of the DNA band in the 240-300 nm region. Both the short and long axes of the pyrene residues of 1-oxiranylpyrene (1-OP) and the (+) and (-) enantiomers of trans-7,8-dihydroxy-anti-9,10-epoxy-7,8,9,10-tetrahydrobenzo[a]pyrene (BPDE) noncovalently bound to double-stranded native DNA are oriented approximately perpendicular to the axis of the DNA helix, consistent with intercalative modes of binding. The covalent binding of these three epoxide derivatives to DNA is accompanied by reorientations of both the short and long axes of the pyrene residues. Covalent adducts derived from the highly mutagenic (+)-anti-BPDE are characterized by tilts of the short axis within 35 degrees or less, and of the long axis by more than 60-80 degrees, with respect to the planes of the DNA bases. In the adducts derived from the binding of the less mutagenic (-)-anti-BPDE and 1-OP epoxide derivatives to DNA, the long axes of the pyrenyl rings are predominantly oriented within 25 degrees of the planes of the DNA bases; however, in the case of the (-) enantiomer of BPDE, there is significant heterogeneity of conformations. In the case of the 1-OP covalent DNA adducts, the short axis of the pyrene ring system is tilted away from the planes of the DNA bases, and the pyrene ring system is not intercalated between DNA base-pairs as in the noncovalent complexes. The stereochemical properties of the saturated 7,8,9,10-ring in BPDE, or the lack of the 7 and 8 carbon atoms in 1-OP, do not seem to affect noncovalent intercalative complex formation which, most likely, is influenced mainly by the flat pyrenyl residues. These structural features, however, strongly influence the conformations of the covalent adducts, which in turn may be responsible for the differences in the mutagenic activities of these molecules.     

Classification of CD and absorption spectra in the Soret band of H(2)TMPyP bound to various synthetic polynucleotides

The binding mode of porphyrins, namely meso-tetrakis(N-methyl pyridinium-4-yl)porphyrin (H(2)TMPyP), was classified in this work by absorption and circular dichroism(CD) spectroscopy. The three binding modes of intercalation, minor groove binding and external stacking exhibit their own characteristic absorption and CD spectra. Intercalation occurs for this porphyrin when bound to GC-rich polynucleotides at a low mixing ratio, as expected. This binding mode produces hypochromism and a red shift in the absorption band and a negative CD band in the Soret absorption region. When it is complexed with AT-rich polynucleotides at a low mixing ratio, hypochromism and a red shift in the absorption band and a positive CD peak is apparent, and this species can easily be assigned to the minor groove-binding mode. For both AT- and GC-rich polynucleotides at a high binding ratio, an excitonic CD was apparent. The sign of excitonic CD depends on the order of the DNA bases; the CD spectra of H(2)TMPyP complexed with non-alternating homopolymer (disregarding the nature of base pairs, i.e. AT or GC) are characterized by a positive band at short wavelengths followed by a negative band at long wavelengths. In contrast, those complexed with alternating polynucleotide were opposite to those of non-alternating homopolymers.     

The interaction of ellipticine derivatives with nucleic acids studied by optical and 1H-nmr spectroscopy: Effect of size of the heterocyclic ring system

The DNA interaction of derivatives of ellipticine with heterocyclic ring systems with three, four, or five rings and a dimethylaminoethyl side chain was studied. Optical spectroscopy of drug complexes with calf thymus DNA, poly [(dA-dT) · (dA-dT)], or poly [(dG-dC) · (dG-dC)] showed a 10 nm bathochromic shift of the light absorption bands of the pentacyclic and tetracyclic compounds upon binding to the nucleic acids, which indicates binding by intercalation. For the tricyclic compound a smaller shift of 1–3 nm was observed upon binding to the nucleic acids. Flow linear dichroism studies show that the geometry of all complexes is consistent with intercalation of the ring system, except for the DNA and poly [(dG-dC) · (dG-dC)] complexes of the tricyclic compound, where the average angle between the drug molecular plane and the DNA helix axis was found to be 65°. One-dimensional ¹H-nmr spectroscopy was used to study complexes between d(CGCGATCGCG)₂ and the tricyclic and pentacyclic compounds. The results on the pentacyclic compound show nonselective broadening due to intermediate chemical exchange of most oligonucleotide resonances upon drug binding. The imino proton resonances are in slow chemical exchange, and new resonances with upfield shifts approaching 1 ppm appear upon drug binding, which supports intercalative binding of the pentacyclic compound. The results on the tricyclic compound show more rapid binding kinetics and very selective broadening of resonances. The data suggest that the tricyclic compound is in an equilibrium between intercalation and minor groove binding, with a preference to bind close to the AT base pairs with the side chain residing in the minor groove. © 1994 John Wiley & Sons, Inc.     

Binding stoichiometry and structure of RecA-DNA complexes studied by flow linear dichroism and fluorescence spectroscopy. Evidence for multiple heterogeneous DNA co-ordination

The interaction between RecA and DNA (in the form of unmodified single-stranded DNA, fluorescent single-stranded DNA and double-stranded DNA) is studied with linear dichroism and fluorescence spectroscopy. RecA is found to form a complex with single-stranded DNA with a binding stoichiometry of about four nucleotides per RecA monomer, in which the DNA bases appear to have a random orientation. Addition of ATP gamma S (a non-hydrolyzable analog of ATP) reduces the stoichiometry to about three nucleotides per RecA and causes the DNA bases to adopt an orientation preferentially perpendicular to the fiber axis. This complex can incorporate an additional strand of single-stranded DNA or double-stranded DNA, yielding a total stoichiometry of six nucleotides or three nucleotides and three base-pairs, respectively, per RecA. RecA, in the presence of ATP gamma S, is also found to interact with double-stranded DNA, with a stoichiometry of about three base-pairs per RecA. In all studied complexes, the tryptophan residues in the RecA protein are oriented with their planes preferentially parallel to the fiber axis, whereas in complexes involving ATP gamma S the planes of the DNA bases are oriented preferentially perpendicular to the fiber. This virtually excludes the possibility that the tryptophan residues are intercalated in the DNA helix. On the basis of these results, a model for the research of homology in the RecA-mediated, strand-exchange reaction in the genetic recombination process is proposed.     

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.     

The cofactor ATP in DNA-RecA complexes is not intercalated between DNA bases

In an attempt to understand the role of ATP as a cofactor at the interaction of the RecA protein with DNA, we have studied the orientation geometries of the cofactor analogs adenosine 5′-O-(3-thiotriphosphate) (ATPγS) and guanosine 5′-O-(3-thiotriphosphate) (GTPγS) in RecA-DNA complexes using flow linear dichroism spectroscopy. Both cofactors promote the formation of RecA-DNA complexes of similar structure as judged from similar orientations of DNA bases. The DNA orientation was probed through the dichroism of the long-wavelength absorption of a DNA analog, poly(dεA). In this way differences between the dichroic spectra of the ATPγS–RecA–DNA and GTPγS-RecA-DNA complexes, observed in the shorter-wavelength region, are related to orientation at variations of the cofactor chromophores. The results show that the guanine plane of GTPγS is oriented parallel with the principal axis of the complex in contrast to the more perpendicular orientation of the DNA bases. This observation directly excludes the possibility that the cofactor could be intercalated between the DNA bases. This observation directly excludes the possibility that the cofactor could be intercalated between the DNA bases. The orientation of the adenine base of ATPγS, which may be similar to that of guanine of GTPγS albeit not exactly the same, is also inconsistent with intercalation. The possibility that the cofactor bound to the protein could be intercalated in DNA had been speculated from the observation that some DNA intercalators can induce RecA binding to DNA in the absence of cofator. There are probably no direct interactions between the cofator and the DNA bases and the role of the cofactor is probably related to interaction with RecA and a modification of protein conformation.     

Stereoselective covalent binding of anti-benzo(a)pyrene diol epoxide to DNA conformation of enantiomer adducts

The conformation of adducts derived from the reactions and covalent binding of the (+) and (-) enantiomers of 7 beta, 8 alpha-dihydroxy-9 alpha, 10 alpha-epoxy-7,8,9,10-tetrahydrobenzo(a)pyrene (anti-BaPDE) with double-stranded calf thymus DNA in vitro were investigated utilizing the electric linear dichroism technique. The linear dichroism and absorption spectra of the covalent DNA complexes are interpreted in terms of a superposition of two types of binding sites. One of these conformations (site I) is a complex in which the plane of the pyrene residue is close to parallel (within 30 degrees) to the planes of the DNA bases (quasi-intercalation), while the other (site II) is an external binding site; this latter type of adduct is attributed to the covalent binding of anti-BaPDE to the exocyclic amino group of deoxyguanine (N2-dG), while site I adducts are attributed to the O6-deoxyguanine and N6-deoxyadenine adducts identified in the product analysis of P. Brookes and M.R. Osborne (Carcinogenesis (1982) 3, 1223-1226). Site II adducts are dominant (approximately 90% in the covalent complexes derived from the (+) enantiomer), but account for only 50 +/- 5% of the adducts in the case of the (-)-enantiomer. The orientation of site II complexes is different by 20 +/- 10 degrees in the adducts derived from the binding of the (+) and the (-) enantiomers to DNA, the long axis of the pyrene chromophore being oriented more parallel to the axis of the DNA helix in the case of the (+) enantiomer. These findings support the proposals by Brookes and Osborne that the difference in spatial orientation of the N2-dG adducts of (-)-anti-BaPDE together with their lower abundance may account for the lower biological activity of the (-) enantiomer. The external site II adducts, rather than site I adducts, appear to be correlated with the biological activity of these compounds.     

Binding geometries of benzo[a]pyrene diol epoxide isomers covalently bound to DNA. Orientational distribution

Flow linear dichroism (LD) of different benzo[a]pyrene diol epoxide (BPDE) isomers covalently bound to calf thymus DNA or poly(dG-dC) provides information about binding geometry and DNA perturbation. With anti-BPDE the apparent angle between the long axis (z) of the pyrene chromophore and the DNA helix axis is approximately 30 degrees as evidenced from the LD of z-polarized absorption bands in the pyrenyl chromophore at 252 and 346 nm. The corresponding angle for the in-plane short axis (y) is determined to be approximately 70 degrees from a y-polarized band at 275 nm. The binding of (+)-anti-BPDE to DNA is found to cause a considerable reduction of the DNA orientation. This is ascribed to a decreased persistence length of DNA, owing either to increased flexibility ("flexible joints") or to permanent kinks at the points of binding. The reduced linear dichroism (LDr), i.e., the ratio between LD and isotropic absorbance, of the long-wavelength absorption band system of BPDE bound to DNA exhibits a wavelength dependence that indicates a relatively wide orientational distribution of the z axis of pyrene. Fluorescence data support the conclusion of a heterogeneous distribution, and a very low polarization anisotropy indicates a mobility between the different orientational states, which is rapid compared to the fluorescence lifetime (nanosecond time scale). Attempts are made to simulate the observed LDr features of the (+)-anti-BPDE-poly(dG-dC) complex using different distribution models on the assumption that the angular dependence of the spectral perturbation is due to dispersive interactions with DNA bases.(ABSTRACT TRUNCATED AT 250 WORDS)     

The complex of ethidium bromide with genomic DNA: structure analysis by polarized Raman spectroscopy

Structural properties of the complex formed between genomic DNA and the intercalating drug ethidium bromide (EtBr) have been determined by use of a Raman microscope equipped with near-infrared laser excitation. The polarized spectra, which were obtained from oriented fibers of the EtBr:DNA complex, are interpreted in terms of the relative orientations of the phenanthridinium ring of EtBr and bases of DNA. Quantification of structure parameters of EtBr and DNA in the complex were assessed using Raman tensors obtained from polarized Raman analyses of oriented specimens of EtBr (single crystal) and DNA (hydrated fiber). We find that the phenanthridinium plane is tilted by 35+/-5 degrees from the plane perpendicular to the fiber (DNA helix) axis. Assuming coplanarity of the phenanthridinium ring and its immediate base neighbors at the intercalation site, such bases would have a tilt angle closer to that of A-DNA (20 degrees) than to that of B-DNA (6 degrees). The average base tilt in stretches of DNA between intercalation sites remains that of B-DNA.     

Binding of meso-tetrakis(N-methylpyridiniumyl)porphyrin isomers to DNA: quantitative comparison of the influence of charge distribution and copper(II) derivatization

Factors influencing the binding of tetracationic porphyrin derivatives to DNA have been comprehensively evaluated by equilibrium dialysis, stopped-flow kinetics, etc., for mesotetrakis (4-N-methylpyridiniumyl)porphyrin [TMpyP (4)]. Technical difficulties have previously precluded a comprehensive study of metalloporphyrins. Since electrostatic interactions with the DNA and metal derivatization of the porphyrins have important consequences, we have investigated in greater detail two isomers of TMpyP (4) (meso-tetrakis(3-N-methylpyridiniumyl)porphyrin, [TMpyP (3)] and meso-tetrakis(2-N-methylpyridiniumyl)porphyrin [TMpyP (2)]) in which the position of the charged centers has been varied. A comprehensive study of the Cu(II) derivatives, e.g., CuTMpyP (4), was possible since the difficulties encountered previously with Ni(II) compounds were not a problem with Cu(II) porphyrins [J. A. Strickland, L. G. Marzilli, M. K. Gay, and W. D. Wilson (1988) Biochemistry 27, 8870-8878]. At 25 degrees C, the apparent equilibrium constants [Kobs] decreased with increasing [Na+] for all porphyrins. The Kobs values were comparable for TMpyP (4) and TMpyP (3) binding to either polyd(G-C).polyd(G-C) [poly[d(G-C)2]] or poly[d(A-T)].poly[d(A-T)] [poly[d(A-T)2]]. For the copper(II) porphyrins, the Kobs values were about fivefold greater. The Kobs value for CuTMpyP (2) binding to poly[d(G-C)2] was too small to measure under typical salt conditions; however, Kobs for binding to poly[d(A-T)2] was about two orders of magnitude smaller than those found for CuTMpyP (4) or CuTMpyP (3). Application of the condensation theory for polyelectrolytes suggests about three charge interactions when CuTMpyP (4), CuTMpyP (3), and TMpyP (3) bind to poly[d(G-C)2] or poly[d(A-T)2], a result comparable to that reported for TMpyP (4). At 20 degrees C and 0.115 M [Na+], incorporation of copper decreased the rates of dissociation from poly[d(A-T)2] by a 100-fold compared to those reported for TMpyP (4) but had little effect on the rates of dissociation from poly[d(G-C)2]. Also, movement of the H3CN+ group from the fourth to the third position of the pyridinium ring enhanced the rates of dissociation from poly[d(A-T)2] but decreased the rates of dissociation from poly[d(G-C)2]. From polyelectrolyte theory, the [Na+] dependence of the dissociation rates from poly[d(G-C)2] is consistent with intercalative binding, while that for poly[d(A-T)2] is consistent with an outside binding model. For calf thymus [CT] DNA at 20 degrees C, a greater decrease in the AT than in the GC imino 1H-nmr signal was observed upon addition of CuTMpyP (2), suggesting selective outside binding to the AT regions.(ABSTRACT TRUNCATED AT 400 WORDS)     

Interaction of DNA with actinocin amides containing cationoid centers in the amide groups

Complexes of DNA with actinocin derivatives containing ω-dialkylaminoalkyl groups in the1 and/or 9 positions of the chromophore were studied by spectrophotometric titration, circular dichroism, and viscometry. Induced circular dichroism (ICD) spectra of the DNA-ligand complexes were compared for the cases of the complexes of known structure established by other methods. It was shown that the presence of an isoelliptic point in the long-wavelength absorption band of the ICD spectra of the ligand under monomeric binding conditions could indicate intercalation of the actinocin chromophore into DNA. The separation of the cationoid center and the chromosphore upon elongation of the methylene chain increases the aggregability of the ligand pn the surface of the DNA double helix, which prevents the intercalation of the chromophore.     

Neocarzinostatin chromophore binds to deoxyribonucleic acid by intercalation

The nonprotein chromophore of neocarzinostatin was found to share many of the characteristics of classical intercalators in its interaction with DNA. Viscosity studies with PM2 DNA indicated that the DNA helix unwinding induced by the chromophore was 0.82 times that of ethidium or 21 degrees. Electric dichroism of the chromophore--DNA complex showed that each bound chromophore molecule lengthened DNA by 3.3 A and that absorbance transitions of the chromophore at 315--385 nm were oriented approximately parallel to DNA bases, as expected for an intercalated aromatic ring. Binding to DNA induced strong hypochromicity and a pronounced red shift in the absorbance spectrum of the chromophore. Spectrophotometric titrations suggested at least two types of chromophore binding sites on DNA; one type of site was saturated at rb = 0.125 chromophore molecule/nucleotide, but binding to additional sites continued to at least rb = 0.3. These physical--chemical studies were performed at pH 4--5 in order to keep the chromophore stable, but chromophore bound to an excess of DNA at pH 7 showed a stable absorbance spectrum identical with that seen at pH 4--5, suggesting that a similar type of binding occurs at neutral pH. Chromophore which had spontaneously degraded in pH 8 buffer did not bind to DNA at all, as judged by absorbance spectroscopy. The degree of protection afforded by DNA against spontaneous chromophore degradation implied a dissociation constant of approximately 5 microM for the DNA--chromophore complex at neutral pH and physiological ionic strength. Supercoiled DNA was nearly twice as effective as relaxed DNA in protecting chromophore from degradation, providing additional evidence for intercalation at neutral pH. Comparison of absorbance, fluorescence, and dichroism spectra suggests that the naphthalene ring system is the intercalating moiety.     

Linear dichroism characteristics of ethidium-and proflavine-supercoiled DNA complexes

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 electrophoresis 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 intercalation 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.(ABSTRACT TRUNCATED AT 400 WORDS)     

Characterization of interaction between DNA and 4',6-diamidino-2-phenylindole by optical spectroscopy

We have examined the interaction between 4',6-diamidino-2-phenylindole (DAPI) and DNA using flow linear dichroism (LD), circular dichroism (CD), and fluorescence techniques. We show the presence of two spectroscopically distinct binding sites at low binding ratios with saturation values of 0.025 and 0.17, respectively. In both sites DAPI is bound with its long axis approximately parallel to the grooves of the DNA helix. Resolution of CD spectra shows that an exciton component is present at higher binding ratios, which we attribute to the interaction of two accidentally close-lying DAPI molecules. We also find evidence that DAPI, at least in the high-affinity site, binds preferentially to AT-rich regions. From the spectroscopic results, supported by structural considerations, we can completely exclude that DAPI is bound to DNA by intercalation. Binding geometries and site densities are consistent with a location of DAPI in the grooves of DNA, with the high-affinity site most probably in the minor groove.     

Complex of fd gene 5 protein and double-stranded RNA

We report the formation of complexes of the single-stranded DNA binding protein encoded by gene 5 of fd virus, with natural double-stranded RNAs. In the first direct visualization of a complex of the fd gene 5 protein with a double-stranded nucleic acid, we show by electron microscopy that the double-stranded RNA complex has a structure which is distinct from that of complexes with single-stranded DNA and is consistent with uniform coating of the exterior of the double-stranded RNA helix by the protein. Circular dichroism spectral data demonstrate that the RNA double helix in the complex is undisrupted, and that perturbation of the 228-nm circular dichroism assigned to protein tyrosines can occur in the absence of intercalation of nucleotide bases with protein aromatic residues. Our findings emphasize the potential importance of interaction with the sugar-phosphate polynucleotide backbone in binding of the fd gene 5 protein to nucleic acids.     

Anomalous excitonic CD of meso-tetrakis(3-N-methylpyridiniumyl)porphyrin bound to poly[d(A-T)(2)

When meso-tetrakis(3-N-methylpyridiniumyl)porphyrin (m-TMPyP) formed a complex with poly[d(A-T)(2)], an intense bisignate excitonic CD in the Soret absorption region was observed. The excitonic CD of the m-TMPyP-poly[d(A-T)(2)] complex is unique in that no other combination of the related porphyrin, namely, meso-tetrakis(n-N-methylpyridiniumyl)porphyrin (where n = 2, 4), and polynucleotide including calf thymus DNA, poly[d(G-C)(2)], poly[d(I-C)(2)], and poly(dA).poly(dT), exhibits a comparable CD spectrum. From the [drug]/[DNA] ratio-dependence of the intensity and the shape of the CD spectrum, this porphyrin species is assigned to an extensively aggregated form. The extensively aggregated porphyrin disperses in 1 h after mixing to form moderately stacked porphyrin at a low mixing ratio. The magnitude of linear dichroism of the extensively aggregated porphyrin was small and the sign was negative in the Soret band, which indicated that the molecular plane of porphyrin in the complex is strongly tilted. On the other hand, the molecular plane of porphyrin is almost parallel to the DNA base plane (perpendicular to the DNA helix axis) in the moderately stacked form.     

Effect of N-alkyl substituents on the DNA binding properties of meso-tetrakis (4-N-alkylpyridinium-4-yl)porphyrins and their nickel derivatives

Resonance Raman, NMR, and visible spectroscopies, as well as viscosity and equilibrium dialysis studies were used to assess the effect of the N-alkyl substituent of meso-tetrakis(4-N-alkylpyridinium-4-yl)porphyrin cations on DNA binding. The DNAs studied include the native DNA, calf thymus DNA (CT DNA), the synthetic polynucleotides [poly(dGdC)]2 and [poly(dAdT)]2, and the oligonucleotide d(TATACGTATA)2. Both the porphyrins and the metalloporphyrins containing Ni(II) were examined with the N-alkyl = propyl (TPrpyP(4) and NiTPrpyP(4)) and 2-hydroxyethyl (TEtOHpyP(4) and NiTEtOHpyP(4)). The results were compared to those from the parent porphyrins with the N-methyl substituent (TMpyP(4) and NiTMpyP(4)). For almost all the comparisons made, the new porphyrin cations gave results very similar to those for the TMpyP(4) species. The resonance Raman study indicated that for the three DNA polymers all the Ni species were in the four-coordinate form when bound to all three polymers. It is suggested that both TPrpyP(4) and TEtOHpyP(4) bind to GC regions of DNA in the same intercalative manner as TMpyP(4) with the N-alkyl substituent extended into the solvent. For AT regions of DNA, the binding of TPrpyP(4) and TEtOHpyP(4) is nonintercalative, as found previously for TMpyP(4). The NiPrpy(4) and NiTEtOHpyP(4) cations bind to these polymers in a similar manner to the apo-porphyrins. The similar Raman spectral changes for the three Ni porphyrins upon addition of [poly(dAdT)]2 suggest that partial intercalation is not occurring because models indicate that it would be difficult to accommodate the bulkier N-alkyl substituents.