Structure of a RecA-DNA complex from linear dichroism and small-angle neutron-scattering in flow-oriented solution

Small-angle neutron-scattering (SANS) and ultraviolet linear dichroism (l.d.) were measured on identical samples of a RecA-double-stranded (ds) DNA complex, including cofactor adenosine 5'-O-thiotriphosphate, which were aligned by flow in two equivalent Couette devices made of niobium and silica, transparent to neutrons and to ultraviolet light, respectively. The SANS anisotropy indicates a modest orientation of the RecA-dsDNA fiber with the helix axis parallel to the flow field. By correlation with the corresponding l.d. of the DNA at the same orientation conditions, it is inferred that the DNA bases have a local orientation that is approximately perpendicular to the helix axis. By comparison with the worse orientation in single-stranded DNA-RecA, this conclusion suggests that the dsDNA in its complex with RecA is not strand separated, and may be accommodated as an essentially unperturbed, straight double helix running along the RecA polymer fiber. The SANS anisotropy is also found to support the assignment of a subsidiary intensity maximum as originating from the pitch of a helical fiber.     

Effect of a conjugated acridine moiety on the binding and reactivity of Cu(II)[9-acridinylmethyl-1,4,7-triazacyclononane] with DNA

The DNA binding orientation and dynamic behavior of Cu(II) complexes of 1,4,7-triazacyclononane ([9]aneN(3)), 1, and an acridine conjugate, 2, were investigated by DNA fiber EPR (EPR=electron paramagnetic resonance) spectroscopy. Crystal and molecular structure of 2 were determined by X-ray diffraction. It has been shown that 1 binds to DNA in two different modes at room temperature; one species is rapidly rotating and the other is immobilized randomly on the DNA. The introduction of acridine to [9]aneN(3) fixed the [Cu([9]aneN(3))](2+) moiety of 2 in two different environments on the DNA: the g(mid R:mid R:) axis of one species (g( parallel)=2.26) is aligned perpendicularly to the DNA fiber axis whereas that of the other (g( parallel)=2.24) aligns<90 degrees with the DNA fiber axis. The different DNA binding structures of 1 and 2 are reflected also in their different efficiencies of DNA cleavage; 2 was found to be more effective both in oxidative and hydrolytic cleavage reactions.     

Toward an understanding of the role of DNA adduct conformation in defining mutagenic mechanism based on studies of the major adduct (formed at N(2)-dG) of the potent environmental carcinogen, benzo[a]pyrene

The process of carcinogenesis is initiated by mutagenesis, which often involves replication past damaged DNA. One question - what exactly is a DNA polymerase seeing when it incorrectly copies a damaged DNA base (e.g., inserting dATP opposite a dG adduct)? - has not been answered in any case. Herein, we reflect on this question, principally by considering the mutagenicity of one activated form of benzo[a]pyrene, (+)-anti-B[a]PDE, and its major adduct [+ta]-B[a]P-N(2)-dG. In previous work, [+ta]-B[a]P-N(2)-dG was shown to be capable of inducing>95% G-->T mutations in one sequence context (5'-TGC), and approximately 95% G-->A mutations in another (5'-AGA). This raises the question - how can a single chemical entity induce different mutations depending upon DNA sequence context? Our current working hypothesis is that adduct conformational complexity causes adduct mutational complexity, where DNA sequence context can affect the former, thereby influencing the latter. Evidence supporting this hypothesis was discussed recently (Seo et al., Mutation Res. [in press]). Assuming this hypothesis is correct (at least in some cases), one goal is to consider what these mutagenic conformations might be. Based on molecular modeling studies, 16 possible conformations for [+ta]-B[a]P-N(2)-dG are proposed. A correlation between molecular modeling and mutagenesis work suggests a hypothesis (Hypothesis 3): a base displaced conformation with the dG moiety of the adduct in the major vs. minor groove gives G-->T vs. G-->A mutations, respectively. (Hypothesis 4, which is a generalized version of Hypothesis 3, is also proposed, and can potentially rationalize aspects of both [+ta]-B[a]P-N(2)-dG and AP-site mutagenesis, as well as the so-called "A-rule".) Finally, there is a discussion of how conformational complexity might explain some unusual mutagenesis results that suggest [+ta]-B[a]P-N(2)-dG can become trapped in different conformations, and why we think it makes sense to interpret adduct mutagenesis results by modeling ds-DNA (at least in some cases), even though the mutagenic event must occur at a ss/ds-DNA junction in the presence of a DNA polymerase.     

GFP-tagged regulatory light chain monitors single myosin lever-arm orientation in a muscle fiber

Myosin is the molecular motor in muscle-binding actin and executing a power stroke by rotating its lever arm through an angle of approximately 70 degrees to translate actin against resistive force. A green fluorescent protein (GFP)-tagged human cardiac myosin regulatory light chain (HCRLC) was constructed to study in situ lever arm orientation one molecule at a time by polarized fluorescence emitted from the GFP probe. The recombinant protein physically and functionally replaced the native RLC on myosin lever arms in the thick filaments of permeabilized skeletal muscle fibers. Detecting single molecules in fibers where myosin concentration reaches 300 microM is accomplished using total internal reflection fluorescence microscopy. With total internal reflection fluorescence, evanescent field excitation, supercritical angle fluorescence detection, and CCD detector pixel size limits detection volume to just a few attoliters. Data analysis manages both the perturbing effect of the TIR interface on probe emission and the effect of high numerical aperture collection of light. The natural myosin concentration gradient in a muscle fiber allows observation of fluorescence polarization from C-term GFP-tagged HCRLC exchanged myosin from regions in the thick filament containing low and high myosin concentrations. In rigor, cross-bridges at low concentration at the end of the thick filament maintain GFP dipole moments at two distinct polar angles relative to the fiber symmetry axis. The lower angle, where the dipole is nearly parallel to fiber axis, is more highly populated than the alternative, larger angle. Cross-bridges at higher concentration in the center of the thick filament are oriented in a homogeneous band at approximately 45 degrees to the fiber axis. The data suggests molecular crowding impacts myosin conformation, implying mutual interactions between cross-bridges alter how the muscle generates force. The GFP-tagged RLC is a novel probe to assess single-lever-arm orientation characteristics in situ.     

Computational and experimental investigation of local stress fiber orientation in uniaxially and biaxially constrained microtissues

The orientation of cells and associated F-actin stress fibers is essential for proper tissue functioning. We have previously developed a computational model that qualitatively describes stress fiber orientation in response to a range of mechanical stimuli. In this paper, the aim is to quantitatively validate the model in a static, heterogeneous environment. The stress fiber orientation in uniaxially and biaxially constrained microscale tissues was investigated using a recently developed experimental system. Computed and experimental stress fiber orientations were compared, while accounting for changes in orientation with location in the tissue. This allowed for validation of the model, and additionally, it showed how sensitive the stress fiber orientation in the experimental system is to the location where it is measured, i.e., the heterogeneity of the stress fiber orientation. Computed and experimental stress fiber orientations showed good quantitative agreement in most regions. A strong local alignment near the locations where boundary conditions were enforced was observed for both uniaxially and biaxially constrained tissues. Excepting these regions, in biaxially constrained tissues, no preferred orientation was found and the distribution was independent of location. The stress fiber orientation in uniaxially constrained tissues was more heterogeneous, and stress fibers mainly oriented in the constrained direction or along the free edge. These results indicate that the stress fiber orientation in these constrained microtissues is mainly determined by the local mechanical environment, as hypothesized in our model, and also that the model is a valid tool to predict stress fiber orientation in heterogeneously loaded tissues.     

Linear dichroism study of RecA-DNA complexes. Structural evidence and binding stoichiometries

In the presence of RecA single-stranded DNA (ssDNA) is found to exhibit flow linear dichroism (LD). In the absence of the cofactor ATP gamma S, the LD is positive with a maximum at about 280 nm, whereas in the presence of the cofactor ATP gamma S there is still a positive long-wavelength band, but a negative LD contribution centered at 260 nm indicates an orientation of the DNA bases preferentially perpendicular to the fiber axis. For the complex between ssDNA and RecA without ATP gamma S, essentially all LD derives from the protein (tryptophane) subunits indicating a structure in which the tryptophanes are preferentially parallel to the fiber axis of the complex while the DNA bases remain essentially unoriented. The magnitude of the LD increases with the RecA/DNA ratio to a point corresponding to approximately three nucleotides per RecA and decreases thereafter with excess of DNA. This indicates that there are two modes of binding with different stoichiometries.     

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.     

Toward an understanding of the role of DNA adduct conformation in defining mutagenic mechanism based on studies of the major adduct (formed at N-dG) of the potent environmental carcinogen, benzo[a]pyrene

The process of carcinogenesis is initiated by mutagenesis, which often involves replication past damaged DNA. One question — what exactly is a DNA polymerase seeing when it incorrectly copies a damaged DNA base (e.g., inserting dATP opposite a dG adduct)? — has not been answered in any case. Herein, we reflect on this question, principally by considering the mutagenicity of one activated form of benzo[a]pyrene, (+)-anti-B[a]PDE, and its major adduct [+ta]-B[a]P-N²-dG. In previous work, [+ta]-B[a]P-N²-dG was shown to be capable of inducing>95% G→T mutations in one sequence context (5′-T C), and 95% G→A mutations in another (5′-A A). This raises the question — how can a single chemical entity induce different mutations depending upon DNA sequence context? Our current working hypothesis is that adduct conformational complexity causes adduct mutational complexity, where DNA sequence context can affect the former, thereby influencing the latter. Evidence supporting this hypothesis was discussed recently (Seo et al., Mutation Res. [in press]). Assuming this hypothesis is correct (at least in some cases), one goal is to consider what these mutagenic conformations might be. Based on molecular modeling studies, 16 possible conformations for [+ta]-B[a]P-N²-dG are proposed. A correlation between molecular modeling and mutagenesis work suggests a hypothesis (Hypothesis 3): a base displaced conformation with the dG moiety of the adduct in the major vs. minor groove gives G→T vs. G→A mutations, respectively. (Hypothesis 4, which is a generalized version of Hypothesis 3, is also proposed, and can potentially rationalize aspects of both [+ta]-B[a]P-N²-dG and AP-site mutagenesis, as well as the so-called “A-rule”.) Finally, there is a discussion of how conformational complexity might explain some unusual mutagenesis results that suggest [+ta]-B[a]P-N²-dG can become trapped in different conformations, and why we think it makes sense to interpret adduct mutagenesis results by modeling ds-DNA (at least in some cases), even though the mutagenic event must occur at a ss/ds-DNA junction in the presence of a DNA polymerase.     

Fluorescence anisotropy of DNA/DAPI complex: torsional dynamics and geometry of the complex.

Fluorescence depolarization of synthetic polydeoxynucleotide/4'-6-diamidino-2-phenylindole dihydrochloride complexes has been investigated as a function of dye/polymer coverage. At low coverage, fluorescence depolarization is due to local torsional motions of the DNA segment where the dye resides. At relatively high coverage, fluorescence depolarization is dominated by energy transfer to other dye molecules along the DNA. The extent of the observed depolarization due to torsional motion depends on the angle the dye molecule forms with the DNA helical axis. A large torsional motion and a small angle produce the same depolarization as a small torsional motion and a large projection angle. Furthermore, the extent of transfer critically depends on the relative orientation of dye molecules along the DNA. The effect of multiple transfer is examined using a Monte Carlo approach. The measurement of depolarization with transfer, at high coverage, allows determination of the dye orientation about the DNA helical axis. The value of the torsional spring constant is then determined, at very low coverage, for few selected polydeoxynucleotides.     

The hand of the helix of deoxyhemoglobin S fibers.

Electron micrographs of deoxyhemoglobin S fiber cross sections provide an end-on view of the fiber whose appearance is sensitive to small changes in orientation. We have developed a procedure to exploit this sensitivity in order to determine the hand of these particles. In a sickle hemoglobin fiber the hemoglobin molecules form long pitch helical strands which twist about the particle axis with a pitch of about 3000 A. Tilting a 400-A-thick cross section by a few degrees aligns one of the long pitch helices so that it is nearly parallel to the direction of view. When a strand of hemoglobin molecules in a fiber is aligned in this manner it appears as a strongly contrasted bright spot. It is this spot, rather than the fiber axis, which appears to be the apparent center of rotation of the cross section. The direction of the displacement of the spot from the particle axis depends upon the particle hand and tilt direction. We have used this property to determine that sickle hemoglobin fibers are right-handed particles. This method may be applicable to other particles with long pitch helices as well.     

Binding to cisplatin-modified DNA by the Saccharomyces cerevisiae HMGB protein Nhp6A

Nhp6A is an abundant non-histone chromatin-associated protein in Saccharomyces cerevisiae that contains a minor groove DNA binding motif called the HMG box. In this report, we show that Nhp6Ap binds to cisplatin intrastrand cross-links on duplex DNA with a 40-fold greater affinity than to unmodified DNA with the same sequence. Nevertheless, Nhp6Ap bound to cisplatinated DNA readily exchanges onto unmodified DNA. Phenanthroline-copper footprinting and two-dimensional NMR on complexes of wild-type and mutant Nhp6Ap with DNA were employed to probe the mode of binding to the cisplatin lesion. Recognition of the cisplatin adduct requires a surface-exposed phenylalanine on Nhp6Ap that promotes bending of DNA by inserting into the helix from the minor groove. We propose that Nhp6Ap targets the cisplatin adduct by means of intercalation by the phenylalanine and that it can bind in either orientation with respect to the DNA lesion. A methionine, which also inserts between base pairs and functions in target selection on unmodified DNA, plays no apparent role in recognition of the cisplatin lesion. Basic amino acids within the N-terminal arm of Nhp6Ap are required for high-affinity binding to the cisplatin adduct as well as to unmodified DNA. Cisplatin mediates its cytotoxicity by forming covalent adducts on DNA, and we find that Deltanhp6a/b mutants are hypersensitive to cisplatin in comparison with the wild-type strain. In contrast, Deltanhp6a/b mutants are slightly more resistant to hydrogen peroxide and ultraviolet irradiation. Therefore, Nhp6A/Bp appears to directly or indirectly function in yeast to enhance cellular resistance to cisplatin.     

Mapping the binding site of aflatoxin B1 in DNA: molecular modeling of the binding sites for the N(7)-guanine adduct of aflatoxin B1 in different DNA sequences

Aflatoxin B1 (AFB1), a potent mutagen and carcinogen, forms an adduct exclusively at the N(7) position of guanine, but the structure of this adduct in double stranded DNA is not known. Molecular modeling (using the program, PSFRODO) in conjunction with molecular mechanical calculation (using the program, AMBER) are used to assess the binding modes available to this AFB1 adduct. Two modes appear reasonable; in one the AFB1 moiety is intercalated between the base pair containing the adducted guanine and the adjacent base pair on the 5'-side in reference to the adducted guanine, while in the second it is bound externally in the major groove of DNA. Rotational flexibility appears feasible in the latter providing four, potential binding sites. Molecular modeling reveals that the binding sites around the reactive guanine in different sequences are not uniformly compatible for interaction with AFB1. As the sequence is changed, one particular external binding site would be expected to give a pattern of reactivities that is reasonably consistent with the observed sequence specificity of binding that AFB1 shows in its reaction with DNA (Benasutti, M., Ejadi, S., Whitlow, M. D. and Loechler, E. L. (1988) Biochemistry 27, 472-481). The AFB1 moiety is face-stacked in the major groove with its long axis approximately perpendicular to the helix axis. Favorable interactions are formed between exocyclic amino groups that project into the major groove on cytosines and adenines surrounding the reactive guanine, and oxygens in AFB1; unfavorable interactions involve van der Waals contacts between the methyl group on thymine and the AFB1 moiety. "Some of the sequence specificity of binding data can be rationalized more readily if it is assumed that 5'-GG-3' sequences adopt an A-DNA structure." Based upon molecular modeling/potential energy minimization calculation, it is difficult to predict how reactivity would change in different DNA sequences in the case of the intercalative binding mode; however, several arguments suggest that intercalation might not be favored. From these considerations a model of the structure for the transition state in reaction of AFB1 with DNA is proposed involving one particular external binding site.     

Orientation of non-blue cupric complexes on DNA fibers.

Three different orientations of non-blue, type 2 cupric complexes on DNA fibers are obtained from EPR data. The cupric complex of bleomycin, CuBlm, binds as described previously (Shields, H., McGlumphy,C., and Hamrick, P., J., Jr. (1982) Biochim. Biophys. Acta 697, 113-120), except possibly with more restricted motion. The square plane of CuBlm makes an angle of about 65 degrees with the fiber axis. The tridentate complex 2-formylpyridine monothiosemicarbazonato Cu2+ binds with its planar structure perpendicular to the fiber axis. In contrast, other tridentate cupric complexes of tripeptides, CuGHK and CuGHG, bind with the square plane parallel to the fiber axis. The bound forms of Cu(GHK) and Cu(GHG) are determined mostly by the GH moiety in the complex; the contribution of lysine in defining the orientation of the copper moiety is minimal. Thus, the structure of the ligand determines the orientation of these complexes on DNA.     

Relating myocardial laminar architecture to shear strain and muscle fiber orientation

Cardiac myofibers are organized into laminar sheets about four cells thick. Recently, it has been suggested that these layers coincide with the plane of maximum shear during systole. In general, there are two such planes, which are oriented at +/-45 degrees to the main principal strain axes. These planes do not necessarily contain the fiber axis. In the present study, we explicitly added the constraint that the sheet planes should also contain the muscle fiber axis. In a mathematical analysis of previously measured three-dimensional transmural systolic strain distributions in six dogs, we computed the planes of maximum shear, adding the latter constraint by using the also-measured muscle fiber axis. Generally, for such planes two solutions were found, suggesting that two populations of sheet orientation may exist. The angles at which the predicted sheets intersected transmural tissue slices, cut along left ventricular short- or long-axis planes, were strikingly similar to experimentally measured values. In conclusion, sheets coincide with planes of maximum systolic shear subject to the constraint that the muscle fiber axis is contained in this plane. Sheet orientation is not a unique function of the transmural location but occurs in two distinct populations.     

Packaging of DNA in cricket sperm. A compact mode of DNA packaging

The packaging of DNA in the sperm of the house cricket (Gryllus bimaculatus) was investigated by microscopical and diffraction methods. The principle of DNA packaging in the cricket sperm is parallel bundling. This is in contrast with that in somatic cells, which assumes successive supercoiling. About 240 threads of DNA are bundled into one 300 A fiber, and then more than 200 fibers (300 A) are packed in a parallel manner in one nucleus. Therefore, DNA is oriented so that its helix axis is parallel with the long axis of the nucleus. This simple packaging of DNA is maintained by a newly discovered protein, 17 K protein; no histones were found. The packaging ratio (the ratio of the volume of DNA to that of the suprastructure) of the chromatin is about 1 and shows an effectiveness much higher than that of the nucleosome solenoid structure. The mode of packaging DNA in cricket sperm is different from the nucleosome structure, and is a quite new type of packaging.     

Investigation of DNA structural changes by infrared spectroscopy

DNA-oriented samples of various origins were studied under different conditions of humidiity and sodium chloride content by means of infrared spectroscopy. (1) Oriented DNA (M. Lysodeikticus, E. coli, calf thymus and salmon sperm) films at 3–4% sodium chloride yield polarized spectra which show drastic changes at relative humidities (r.h.) between 94% and 0% indicative of conformational changes: B form → a form → disordered form The measurements of the infrared dichroism at frequencies of about 1230 cm^?1 and at about 1090 cm^?1 allow one to determine the orientation of the phosphate group, whereas the measurements at 1710 cm^?1 characterize the base orientation. At humidities higher than 90% r.h. (B form) the bisector of OPO forms an angle of 70° relative to the helix axis, whereas at lower humidities, between 75% and 50% r.h. (A form) a rotation to about 45° is observed. Simultaneously, the 0—0 line of phosphate group changes its orientation from 55° to 65° to the helix when B → A transition takes place. The results are in general agreement with that of X-ray diffraction and allow one to determine the orientation of the phosphate group with greater precision. (2) The B–A conformational change is not observed for satellite DNA, isolated from Cancer pagurus, of which the guanine + cytosine content is below 5%. As a function of decreasing humidities, one observes the transition: B form → disordered form A diagram of conformational changes of DNA's as a function of base composition and of r.h., suggests that B–A transition will occur for DNA of relatively higher G + C content, whereas for high (A + T) content, base sequence may be of importance. The B–A transition is prevented in DNA at a relatively high or very low sodium chloride content.     

Computer simulation of the 30-nanometer chromatin fiber

A new Monte Carlo model for the structure of chromatin is presented here. Based on our previous work on superhelical DNA and polynucleosomes, it reintegrates aspects of the "solenoid" and the "zig-zag" models. The DNA is modeled as a flexible elastic polymer chain, consisting of segments connected by elastic bending, torsional, and stretching springs. The electrostatic interaction between the DNA segments is described by the Debye-Hückel approximation. Nucleosome core particles are represented by oblate ellipsoids; their interaction potential has been parameterized by a comparison with data from liquid crystals of nucleosome solutions. DNA and chromatosomes are linked either at the surface of the chromatosome or through a rigid nucleosome stem. Equilibrium ensembles of 100-nucleosome chains at physiological ionic strength were generated by a Metropolis-Monte Carlo algorithm. For a DNA linked at the nucleosome stem and a nucleosome repeat of 200 bp, the simulated fiber diameter of 32 nm and the mass density of 6.1 nucleosomes per 11 nm fiber length are in excellent agreement with experimental values from the literature. The experimental value of the inclination of DNA and nucleosomes to the fiber axis could also be reproduced. Whereas the linker DNA connects chromatosomes on opposite sides of the fiber, the overall packing of the nucleosomes leads to a helical aspect of the structure. The persistence length of the simulated fibers is 265 nm. For more random fibers where the tilt angles between two nucleosomes are chosen according to a Gaussian distribution along the fiber, the persistence length decreases to 30 nm with increasing width of the distribution, whereas the other observable parameters such as the mass density remain unchanged. Polynucleosomes with repeat lengths of 212 bp also form fibers with the expected experimental properties. Systems with larger repeat length form fibers, but the mass density is significantly lower than the measured value. The theoretical characteristics of a fiber with a repeat length of 192 bp where DNA and nucleosomes are connected at the core particle are in agreement with the experimental values. Systems without a stem and a repeat length of 217 bp do not form fibers.     

Mutagenesis by site-specific arylamine adducts in plasmid DNA: enhancing replication of the adducted strand alters mutation frequency

Site specifically modified plasmids were used to determine the mutagenic effects of single arylamine adducts in bacterial cells. A synthetic heptadecamer bearing a single N-(guanin-8-yl)-2-aminofluorene (AF) or N-(guanin-8-yl)-2-(acetylamino)fluorene (AAF) adduct was used to introduce the adducts into a specific site in plasmid DNA that contained a 17-base single-stranded region complementary to the modified oligonucleotide. Following transformation of bacterial cells with the adduct-bearing DNA, putative mutants were detected by colony hybridization techniques that allowed unbiased detection of all mutations at or near the site of the adduct. The site-specific AF or AAF adducts were also placed into plasmid DNA that contained uracil residues on the strand opposite that bearing the lesions. The presence of uracil in one strand of the DNA decreases the ability of the bacterial replication system to use the uracil-containing strand, thereby favoring the use of the strand bearing the adducts. In a comparison of the results obtained with site specifically modified DNA, either with or without uracil, the presence of the uracil increased the mutation frequencies of the AF adduct by greater than 7-fold to 2.9% and of the AAF adduct by greater than 12-fold to 0.75%. The mutation frequency of the AF adduct was greatly reduced in a uvrA- strain while no mutations occurred with the AAF adduct in this strain. The sequence changes resulting from these treatments were dependent on adduct structure and the presence or absence of uracil on the strand opposite the adducts.(ABSTRACT TRUNCATED AT 250 WORDS)     

In vitro DNA and dGMP adducts formation caused by ochratoxin A

Ochratoxin A (OTA), a nephrotoxic and nephrocarcinogenic mycotoxin, leads to the formation of DNA adducts after administration to animals. This could be due to an epigenetic effect. In vitro assays can exclude an indirect effect, where the xenobiotic can generate, in vivo, endogenous reactive compounds which give adducts on DNA. Microsomes prepared from mice or rabbit kidney and liver, used as metabolic activators, were incubated in the presence of commercial salmon testes DNA and OTA, with NADPH or arachidonic acid used as cofactors. Upto 126 DNA adducts for 10(9) nucleotides were detected using the 32P postlabeling method after incubation with the mouse kidney system. Similar results were obtained with rabbit kidney microsomes. Using liver microsomes, the number of DNA adducts detected was much lower. When NADPH was used as a cosubstrate (to explore the cytochrome P450 metabolic pathways), with mice kidney microsomes, the adduct level was only 44% of the one obtained with arachidonic acid. These results lend support to the hypothesis of the preferential activation of OTA by the peroxidase activity of prostaglandin synthases and/or lipoxygenases to direct genotoxic metabolites, and are in agreement with the previously obtained results after in vivo treatment of mice. In order to identify the nucleotides of DNA modified by the OTA metabolites, dAMP, dGMP, dTMP and dCMP were used as substrates under the same conditions as with DNA. The adducts were found only on dGMP. The total adduct level was of 344 adducts per 10(9) nucleotides with the appearance of three major adducts in the presence of arachidonic acid. With NADPH, 271 adducts were obtained per 10(9) nucleotides, with again three major adducts, but only two of them were similar to two adducts obtained in the presence of arachidonic acid. Desferal (desferrioxamine B methanesulphonate), at a 50 microM concentration, did not reduce the adduct level. Adducts were also obtained when polydG, polydC and dG-p-dG were used as alternative substrates, whereas no adducts were obtained with polydA, polydT and polydC. The major adduct obtained after incubation of DNA with OTA, comigrated with the major adduct obtained with dGMP, in two chromatographic solvents. These results show that OTA is metabolized to genotoxic metabolite(s) which interact with the guanine residues of DNA.     

Interaction of benz[a]pyrene diol epoxide with chromatin studied by flow linear dichroism

Chromatin isolated from Ehrlich ascites cells was incubated with the tumourigenic compound (+)-7 beta,8 alpha-dihydroxy-9 alpha,10 alpha-epoxy-7,8,9,10- tetrahydrobenz[a]pyrene [(+)-anti-BPDE] at low ionic strength and the modified chromatin was analysed using flow linear dichroism (LD). The results confirm that (+)-anti-BPDE preferentially binds to the DNA in the linker regions, and furthermore show that the long axis of the bound pyrenyl chromophore is oriented parallel or close to parallel to the average orientation of the chromatin fiber axis. The data indicate that the binding geometry of (+)-anti-BPDE in chromatin is similar to that in pure DNA and deoxyguanosine-containing double-helical oligonucleotides.