Superhelix Density Research Articles

DNA damage modeled with Geant4-DNA: effects of plasmid DNA conformation and experimental conditions

The chemical stage of the Monte Carlo track-structure (MCTS) code Geant4-DNA was extended for its use in DNA strand break (SB) simulations and compared against published experimental data. Geant4-DNA simulations were performed using pUC19 plasmids (2686 base pairs) in a buffered solution of DMSO irradiated by 60Co or 137Cs γ-rays. A comprehensive evaluation of SSB yields was performed considering DMSO, DNA concentration, dose and plasmid supercoiling. The latter was measured using the super helix density value used in a Brownian dynamics plasmid generation algorithm. The Geant4-DNA implementation of the independent reaction times method (IRT), developed to simulate the reaction kinetics of radiochemical species, allowed to score the fraction of supercoiled, relaxed and linearized plasmid fractions as a function of the absorbed dose. The percentage of the number of SB after •OH + DNA and H• + DNA reactions, referred as SSB efficiency, obtained using MCTS were 13.77% and 0.74% respectively. This is in reasonable agreement with published values of 12% and 0.8%. The SSB yields as a function of DMSO concentration, DNA concentration and super helix density recreated the expected published experimental behaviors within 5%, one standard deviation. The dose response of SSB and DSB yields agreed with published measurements within 5%, one standard deviation. We demonstrated that the developed extension of IRT in Geant4-DNA, facilitated the reproduction of experimental conditions. Furthermore, its calculations were strongly in agreement with experimental data. These two facts will facilitate the use of this extension in future radiobiological applications, aiding the study of DNA damage mechanisms with a high level of detail.

Regulation of the gyr operon of Mycobacterium tuberculosis by overlapping promoters, DNA topology, and reiterative transcription

DNA gyrase introduces negative supercoils into DNA to maintain topological homeostasis. The genes encoding gyrase, gyrB and gyrA, form a dicistronic operon in Mycobacterium tuberculosis (Mtb) and other actinobacteria. Earlier work indicated that DNA relaxation stimulates the expression of the gyr genes, a phenomenon termed relaxation-stimulated transcription (RST). The present study addresses the underlying mechanism of gyr operon regulation. The operon is regulated by overlapping and divergently oriented promoters located upstream of gyrB. The principal promoter, PgyrB1, drives transcription of the operon, while a weak “reverse” promoter, PgyrR, transcribes in opposite direction. We demonstrate that PgyrR plays a role in fine tuning gyr gene expression by reiterative transcription (RT), a regulatory mechanism hitherto not found in Mtb. In vitro transcription assays showed that RT at PgyrR depended on the negatively supercoiled state of the DNA template. The principal promoter, PgyrB1, was also sensitive to DNA supercoiling, but it was stimulated by DNA relaxation. Moreover, RNA polymerase binding to the promoter was efficient at PgyrB1 when template DNA was relaxed, whereas binding to PgyrR was preferred when DNA was supercoiled. Thus, a collaboration between RST and RT governs the regulation of the gyr operon; the differing sensitivity of the two overlapping promoters to superhelix density explains how gyrase expression responds to changes in supercoiling to determine the efficiency of transcription initiation.

Preferential Binding of Hot Spot Mutant p53 Proteins to Supercoiled DNA In Vitro and in Cells

Hot spot mutant p53 (mutp53) proteins exert oncogenic gain-of-function activities. Binding of mutp53 to DNA is assumed to be involved in mutp53-mediated repression or activation of several mutp53 target genes. To investigate the importance of DNA topology on mutp53-DNA recognition in vitro and in cells, we analyzed the interaction of seven hot spot mutp53 proteins with topologically different DNA substrates (supercoiled, linear and relaxed) containing and/or lacking mutp53 binding sites (mutp53BS) using a variety of electrophoresis and immunoprecipitation based techniques. All seven hot spot mutp53 proteins (R175H, G245S, R248W, R249S, R273C, R273H and R282W) were found to have retained the ability of wild-type p53 to preferentially bind circular DNA at native negative superhelix density, while linear or relaxed circular DNA was a poor substrate. The preference of mutp53 proteins for supercoiled DNA (supercoil-selective binding) was further substantiated by competition experiments with linear DNA or relaxed DNA in vitro and ex vivo. Using chromatin immunoprecipitation, the preferential binding of mutp53 to a sc mutp53BS was detected also in cells. Furthermore, we have shown by luciferase reporter assay that the DNA topology influences p53 regulation of BAX and MSP/MST1 promoters. Possible modes of mutp53 binding to topologically constrained DNA substrates and their biological consequences are discussed.

Preferential binding of IFI16 protein to cruciform structure and superhelical DNA

Interferon (IFN)-inducible HIN-200 proteins play an important role in transcriptional regulation linked to cell cycle control, inflammation, autoimmunity and differentiation. IFI16 has been identified as a target of IFNα and γ and is a member of the HIN-200 protein family. Expression level of IFI16 is often decreased in breast cancers, implicating its role as a tumor suppressor. As a potent transcription factor, IFI16 possesses a transcriptional regulatory region, a PYD/DAPIN/PAAD region which associates with IFN response, DNA-binding domains and binding regions for tumor suppressor proteins BRCA1 and p53. It is also reported that IFI16 protein is capable of binding p53 and cMYC gene promoters. Here, we demonstrate that IFI16 protein binds strongly to negatively superhelical plasmid DNA at a native superhelix density, as evidenced by electrophoretic retardation of supercoiled (sc) DNA in agarose gels. Binding of IFI16 to supercoiled DNA results in the appearance of one or more retarded DNA bands on the gels. After removal of IFI16, the original mobility of the scDNA is recovered. By contrast, IFI16 protein binds very weakly to the same DNA in linear state. Using short oligonucleotide targets, we also detect a strong preference for IFI16 binding to cruciform DNA structure compared to linear DNA topology. Hence, this novel DNA-binding property of IFI16 protein to scDNA and cruciform structures may play critical roles in its tumor suppressor function.

Selective binding of tumor suppressor p53 protein to topologically constrained DNA: Modulation by intercalative drugs

Selective binding of the wild type tumor suppressor protein p53 to negatively and positively supercoiled (sc) DNA was studied using intercalative drugs chloroquine ( CQ), ethidium bromide, acridine derivatives and doxorubicin as a modulators of the level of DNA supercoiling. The p53 was found to lose gradually its preferential binding to negatively scDNA with increasing concentrations of intercalators until the DNA negative superhelix turns were relaxed. Formation of positive superhelices (due to further increasing intercalator concentrations) rendered the circular duplex DNA to be preferentially bound by the p53 again. CQ at concentrations modulating the closed circular DNA topology did not prevent the p53 from recognizing a specific target sequence within topologically unconstrained linear DNA. Experiments with DNA topoisomer distributions differing in their superhelix densities revealed the p53 to bind selectively DNA molecules possessing higher number of negative or positive superturns. Possible modes of the p53 binding to the negatively or positively supercoiled DNA and tentative biological consequences are discussed.

The Central Region of BRCA1 Binds Preferentially to Supercoiled DNA

BRCA1 is a multifunctional tumor suppressor protein with implications in regulating processes such as cell cycle, transcription, DNA repair, and chromatin remodeling. The function of BRCA1 likely involves interactions with a vast number of proteins and likewise DNA. To this date there is only fragmentary evidence about BRCA1 binding to DNA. In this study, we provide detailed analyses of various BRCA1 protein constructs binding to linear and super-coiled (sc) DNAs. We demonstrate that the central region of human BRCA1 binds strongly to negatively sc plasmid DNA at a native superhelix density, as evidenced by electrophoretic retardation of sc DNA in agarose gels. At relatively low BRCA1:DNA ratios, binding of BRCA1 to sc DNA results in the appearance of one or more retarded DNA bands on the gels. After removal of BRCA1, the original mobility of the sc DNA is recovered. BRCA1 proteins at higher concentrations also bind to the same DNA but in linear state, leading to formation of a smeared retarded band. Our experiments not only demonstrate a preference for BRCA1 binding to sc DNA, but also show that the central region may contain at least two efficient DNA binding domains with strong affinity for sc DNA. The biological implications of the novel DNA binding activities of BRCA1 are discussed.

DNA topology influences p53 sequence-specific DNA binding through structural transitions within the target sites

The tumour suppressor protein p53 is one of the most important factors regulating cell proliferation, differentiation and programmed cell death in response to a variety of cellular stress signals. P53 is a nuclear phosphoprotein and its biochemical function is closely associated with its ability to bind DNA in a sequence-specific manner and operate as a transcription factor. Using a competition assay, we investigated the effect of DNA topology on the DNA binding of human wild-type p53 protein. We prepared sets of topoisomers of plasmid DNA with and without p53 target sequences, differing in their internal symmetry. Binding of p53 to DNA increased with increasing negative superhelix density (-sigma). At -sigma < or = 0.03, the relative effect of DNA supercoiling on protein-DNA binding was similar for DNA containing both symmetrical and non-symmetrical target sites. On the other hand, at higher -sigma, target sites with a perfect inverted repeat sequence exhibited a more significant enhancement of p53 binding as a result of increasing levels of negative DNA supercoiling. For -sigma = 0.07, an approx. 3-fold additional increase in binding was observed for a symmetrical target site compared with a non-symmetrical target site. The p53 target sequences possessing the inverted repeat symmetry were shown to form a cruciform structure in sufficiently negative supercoiled DNA. We show that formation of cruciforms in DNA topoisomers at -sigma > or = 0.05 correlates with the extra enhancement of p53-DNA binding.

Probability of the Site Juxtaposition Determines the Rate of Protein-Mediated DNA Looping

Numerous biological processes are regulated by DNA elements that communicate with their targets over a distance via formation of protein-bridged DNA loops. One of the first questions arising in studies of DNA looping is whether the rate of loop formation is limited by diffusion of the DNA sites. We addressed this question by comparing the in vitro measured rates of transcription initiation in the NtrC- glnAp2 enhancer-dependent transcription initiation system with predictions of two different theoretical models. The promoter and enhancer were in a 7.6-kb plasmid and separated by 2.5 kb. The measurements were performed for different values of the plasmid superhelix density, from 0 to −0.07. Earlier theoretical analysis, based on the Monte Carlo simulation of DNA conformations, showed that if the rate of loop formation is determined by the equilibrium probability of juxtaposition of the DNA sites, the rate should be ∼100 times higher in supercoiled than in relaxed DNA. On the other hand, Brownian dynamics simulation showed that if the rate of loop formation is limited by the site diffusion, it should be nearly independent of DNA supercoiling. We found that efficiency of the transcription initiation increases by nearly two orders of magnitude as a result of the corresponding increase of the template supercoiling. This clearly shows that the rate of bridging in the enhancer-promoter system is not limited by diffusion of the DNA sites to one another. We argue that this conclusion derived for the specific system is likely to be valid for the great majority of biological processes involving protein-mediated DNA looping.

S-DNA, over-supercoiled DNA with a 1.94-to 2.19-Å rise per base pair

Supercoiled 3993-bp pGEMEX DNA immobilized on four substrates (freshly cleaved mica, standard amino mica, and modified amino mica with an increased or decreased surface charge density in comparison to standard amino mica) has been visualized by atomic force microscopy in the air. Plectonomically supercoiled DNA molecules, as well as single molecules with an extremely high compaction level (i.e., with a significantly higher superhelix density compared to those previously observed experimentally or estimated theoretically), have been visualized on modified amino mica with an increased surface charge density. The distance between nucleotide pairs along the duplex axis has been determined by measuring the contour length of individual oversupercoiled DNA molecules. The estimated rise per base pair varies from 1.94 to 2.19 A. These supercoiled DNA molecules, which are compressed like a spring and have a decreased rise per base pair compared to previously known DNA forms are considered to be a new form of DNA, S-DNA. A model of S-DNA has been constructed. Molecules of S-DNA may be an intermediate in the course of the compaction of single supercoiled DNA molecules into spheroids and minitoroids. The DNA oversupercoiling, followed by the compression of the supercoiled molecules, has been shown to be accounted for by a high surface charge density of amino mica on which DNA molecules are immobilized.

Stress-induced DNA duplex destabilization (SIDD) in the E. coli genome: SIDD sites are closely associated with promoters.

We present the first analysis of stress-induced DNA duplex destabilization (SIDD) in a complete chromosome, the Escherichia coli K12 genome. We used a newly developed method to calculate the locations and extents of stress-induced destabilization to single-base resolution at superhelix density sigma = -0.06. We find that SIDD sites in this genome show a statistically highly significant tendency to avoid coding regions. And among intergenic regions, those that either contain documented promoters or occur between divergently transcribing coding regions, and hence may be inferred to contain promoters, are associated with strong SIDD sites in a statistically highly significant manner. Intergenic regions located between convergently transcribing genes, which are inferred not to contain promoters, are not significantly enriched for destabilized sites. Statistical analysis shows that a strongly destabilized intergenic region has an 80% chance of containing a promoter, whereas an intergenic region that does not contain a strong SIDD site has only a 24% chance. We describe how these observations may illuminate specific mechanisms of regulation, and assist in the computational identification of promoter locations in prokaryotes.

Monte Carlo Simulations of Locally Melted Supercoiled DNAs in 20 mM Ionic Strength

Mesoscopic models of unmelted and locally melted supercoiled DNAs in 20 mM ionic strength are simulated over a range of linking difference from Δ ℓ = 0 to −26 turns, or superhelix density from σ = 0 to −0.062. A domain containing m = 0, 28, or 56 melted basepairs (out of 4349 total) is modeled simply by a region of suitable length with substantially reduced torsion and bending elastic constants. Average structural properties are calculated from the saved configurations, and a reversible work protocol is used to calculate the supercoiling free energy, Δ G sc . The cross-writhe between duplex and melted regions (defined herein) is found to be negligibly small. The total writhe, radius of gyration, and ordered elements of the diagonalized inertial tensor are found to be nearly universal functions of the residual linking difference ( 〈 Δ ℓ r 〉 ) associated with the duplex region, independent of m. However, deformability of the tertiary structure, as manifested by the variance of those same properties, is not a universal function of 〈 Δ ℓ r 〉 , but depends upon m. Δ G sc varies with 〈 Δ ℓ r 〉 more strongly than 〈 Δ ℓ r 〉 2 due to the low ionic strength. The twist energy parameter, E T , obtained from the simulated Δ G sc , 〈 Δ ℓ r 〉 , and net twisting strain of the melted region, 〈 T D 〉 , is found to be independent of m, hence also of the torsion and bending elastic constants of the melted region. However, E T increases linearly with − 〈 Δ ℓ r 〉 , which leads to 1), a small overestimation of E T for any given 〈 Δ ℓ r 〉 , when E T is determined from the observed Δ ℓ and 〈 Δ ℓ r 〉 by the protocol of Bauer and Benham; and 2), a significant enhancement of the apparent slope, ⁡ − ⁡ d E T / d T , obtained via the protocol of Bauer and Benham, relative to the actual slope at fixed 〈 Δ ℓ r 〉 . After taking these two effects into account, the theoretical and experimental E T values and − ⁡ d E T / d T values agree rather well. For the larger Δ ℓ , the melted regions are found preferentially in the linker domains between interwound arms, rather than in the apical regions at the ends of interwound arms.

Role of tumor suppressor p53 domains in selective binding to supercoiled DNA.

We showed previously that bacterially expressed full-length human wild-type p53b(1-393) binds selectively to supercoiled (sc)DNA in sc/linear DNA competition experiments, a process we termed supercoil-selective (SCS) binding. Using p53 deletion mutants and pBluescript scDNA (lacking the p53 recognition sequence) at native superhelix density we demonstrate here that the p53 C-terminal domain (amino acids 347-382) and a p53 oligomeric state are important for SCS binding. Monomeric p53(361-393) protein (lacking the p53 tetramerization domain, amino acids 325-356) did not exhibit SCS binding while both dimeric mutant p53(319- 393)L344A and fusion protein GCN4-p53(347-393) were effective in SCS binding. Supershifting of p53(320-393)-scDNA complexes with monoclonal antibodies revealed that the amino acid region 375-378, constituting the epitope of the Bp53-10.1 antibody, plays a role in binding of the p53(320-393) protein to scDNA. Using electron microscopy we observed p53-scDNA nucleoprotein filaments produced by all the C-terminal proteins that displayed SCS binding in the gel electrophoresis experiments; no filaments formed with the monomeric p53(361- 393) protein. We propose a model according to which two DNA duplexes are compacted into p53-scDNA filaments and discuss a role for filament formation in recombination.

Polycomb group repression reduces DNA accessibility.

The Polycomb group proteins are responsible for long-term repression of a number of genes in Drosophila melanogaster, including the homeotic genes of the bithorax complex. The Polycomb protein is thought to alter the chromatin structure of its target genes, but there has been little direct evidence for this model. In this study, the chromatin structure of the bithorax complex was probed with three separate assays for DNA accessibility: (i) activation of polymerase II (Pol II) transcription by Gal4, (ii) transcription by the bacteriophage T7 RNA polymerase (T7RNAP), and (iii) FLP-mediated site-specific recombination. All three processes are restricted or blocked in Polycomb-repressed segments. In contrast, control test sites outside of the bithorax complex permitted Gal4, T7RNAP, and FLP activities throughout the embryo. Several P insertions in the bithorax complex were tested, providing evidence that the Polycomb-induced effect is widespread over target genes. This accessibility effect is similar to that seen for SIR silencing in Saccharomyces cerevisiae. In contrast to SIR silencing, however, episomes excised from Polycomb-repressed chromosomal sites do not show an altered superhelix density.

An initiation element in the yeast CUP1 promoter is recognized by RNA polymerase II in the absence of TATA box-binding protein if the DNA is negatively supercoiled.

Purified RNA polymerase II initiated transcription from the yeast CUP1 promoter fused to a C-less cassette if the DNA was negatively supercoiled. Relaxed plasmid was not transcribed. Transcription did not require addition of any other transcription factors. TATA box-binding protein (TBP) was not detectable in the polymerase preparation and the TATA box was not required. Deletion analysis of the CUP1 promoter revealed that a 25-bp element containing the initiation region was sufficient for recognition by polymerase. Two transcription start sites were mapped, one of which is identical to one of the two major start sites observed in vivo. Our observations can be accounted for by using a theoretical analysis of the probability of DNA melting within the plasmid as a function of superhelix density: the CUP1 initiation element is intrinsically unstable to superhelical stress, permitting entry of the polymerase, which then scans the DNA to locate the start site. In support of this analysis, the CUP1 promoter was sensitive to mung bean nuclease. These observations and a previous theoretical analysis of yeast genes support the idea that promoters are stress points within the DNA superhelix. The role of transcription factors might be to mark the promoter and to regulate specific melting of promoter DNA.

Two superhelix density-dependent DNA transitions detected by changes in DNA adsorption/desorption behavior.

The adsorption behavior of covalently closed circular plasmid DNA at the mercury/water interface was studied by means of AC impedance measurements. The dependence of the differential capacitance (C) of the electrode double layer on the potential (E) was measured in the presence of adsorbed DNA. It was found that the C-E curves of supercoiled DNA at native and highly negative superhelix densities (sigma), relaxed covalently closed circular DNA, and nicked DNA differed from each other. A detailed study of topoisomer distributions ranging from -sigma of 0 to 0.11 revealed two supercoiling-dependent transitions, at about -sigma = 0.04 (transition TI) and 0.07 (transition TII). Transition TI was detected by measuring the height of the adsorption/desorption peak 1 (at about -1.2 V against the saturated calomel electrode) and the decrease of capacitance (DeltaC) at -0.35 V. This transition may be due to a sudden change in the ability of the DNA to respond to the alternating voltage, probably caused by changes in the DNA tertiary and/or secondary structure. Transition TII was detected by measuring peak 3* (at about -1.3 V), which was absent in topoisomers with -sigma less than 0.05. This transition is due to changes in the DNA adsorption/desorption behavior related to increased accessibility of bases at elevated negative superhelix density. Opening of the duplex at highly negative superhelix density was also detected by the single-strand selective probe of DNA structure, osmium tetroxide, 2, 2'-bipyridine. Our results suggest that electrochemical techniques provide sensitive experimental analysis of changes in DNA structure.

The effect of ionic conditions on the conformations of supercoiled DNA. II. equilibrium catenation

We studied the equilibrium formation of DNA catenanes to assess the conformational properties of supercoiled DNA as a function of ionic conditions and supercoiling density. Catenanes were formed by cyclizing linear DNA with long cohesive ends in the presence of supercoiled molecules. The efficiency of the catenation depends on the distance between opposing segments of DNA in the interwound superhelix. The fraction of cyclizing molecules that becomes topologically linked with the supercoiled DNA is the product of the concentration of the supercoiled DNA and a proportionality constant, B, that depends on conformations of supercoiled DNA. In parallel with these experimental studies, we calculated the values of B using Monte Carlo simulations of the equilibrium distribution of DNA conformations. There were no adjustable parameters in the calculations because all three parameters of the DNA model, bending and torsional elasticity of DNA and DNA effective diameter, specifying intersegment interactions, were known from independent studies. We found very good agreement between measured and simulated values of B for all the ionic conditions and DNA superhelix densities studied; the discrepancy was less than a factor of 2 over the 200-fold variation in B. The value of B decreases nearly exponentially with increasing superhelicity, this dependence being especially strong at low salt concentration. The dependence of B on the concentration of NaCl, MgCl 2, and spermidine can be described with good accuracy in terms of changes of the DNA effective diameter. We found no indication of superhelix collapse under any ionic conditions studied. We discuss, in light of these results, the biological importance of the effect of DNA supercoiling on the unlinking of the products of DNA replication.

Effects of Na +and Mg 2+on the Structures of Supercoiled DNAs: Comparison of Simulations with Experiments

Recent cryo-electron microscopy (cryo-EM) results suggest that sufficient NaCl concentration (≤0.1 M) and superhelix density (≤−0.05) cause circular DNAs to adopt highly extended, tightly interwound configur ations, in which the strands are laterally contiguous along almost their entire length. Millimolar levels of MgCl 2reportedly act synergistically with NaCl to produce similar conformations. However, Monte Carlo simulations with purely repulsive interduplex forces failed to reproduce such structures. In the present work, solution measurements of particular physical properties were performed both to characterize the effects of Na +and Mg 2+on DNA structure and to provide quantitative tests of Monte Carlo simulations of circular DNAs. Supercoiled p30δ DNAs in 10 mM Tris plus 0, 0.122, and 0.1 M NaCl, and 0.1 M NaCl plus 4 mM Mg 2+were examined by static and dynamic light scattering (LS and DLS), time- resolved fluorescence polarization anisotropy (FPA) of intercalated ethidium, and circular dichroism (CD) spectroscopy. Upon addition of 0.122 M NaCl, the radius of gyration ( R g) decreased substantially, which indicates that p30δ adopts a more compact structure. This contradicts the cryo-EM studies, where molecular extension and R gboth increase upon adding 0.1 M NaCl. In 0.1 M NaCl, the torsion constant measured by FPA is practically invariant to superhelix density, and the plateau diffusion coefficient at large scattering vector ( D plat) is likewise nearly the same at both relaxed and native superhelix densities. Such invariance is difficult to reconcile with any transition from relaxed circles to tightly interwound structures with laterally contiguous strands. Metropolis Monte Carlo simulations were performed to generate canonically distributed sets of structures, from which average D 0values and scattered intensity ratios, 〈I(0)〉/〈 I( k)〉, were calculated. Agreement between simulations and experiments in regard to 〈 I(0)|〉/〈 I( k)〉, D 0and the supercoiling free energy, Δ G sc(Δl ), is remarkably good for the most extensively studied p30δ samples. The simulated structures exhibit no sign of very tight interwinding with extensive lateral contacts, but instead exhibit most probable superhelix diameters of 85 to 90 Å. When 4 mM Mg 2+was added to native supercoiled p30δ in 0.1 M NaCl, R gdecreased, D 0increased, and the longest internal relaxation rate (1/τ 2(0)) increased, all of which indicate a further overall contraction of the molecular envelope. The torsion constant exhibited a slight increase that is hardly statistically significant. In this case, agreement between the simulations and experiments was only semi-quantitative for most samples investigated, although the predicted contraction was exhibited by all five samples of p30δ and one of pBR322 DNA. The simulated structures in 0.1 M NaCl plus 4 mM Mg 2+again showed no sign of extensive lateral contacts. A plausible explanation is proposed for the highly extended, tightly interwound structures seen in cryo-EM, and explicitly tested by Monte Carlo simulations of a 1000 bp circular DNA at +25 and −50°C. Structures identical to those seen in cyro-EM are in fact the equilibrium structures in the simulations at −50°C, and the estimated time for equilibration (2.3×10 −6second) is much smaller than the estimated time for vitrification (1×10 −4second).

Enhanced peptide nucleic acid binding to supercoiled DNA: possible implications for DNA "breathing" dynamics.

The influence of DNA topology on peptide nucleic acid (PNA) binding was studied. Formation of sequence-specific PNA2/dsDNA (double-stranded DNA) complexes was monitored by a potassium permanganate probing/primer extension assay. At low ionic strengths, the binding of PNA was 2-3 times more efficient with supercoiled than with linear DNA. In the presence of 140 mM KCI, the PNA binding rate was reduced but, notably, highly dependent on template topology. Negative supercoiling (mean superhelix density, sigma approximately -0.051) increased the rate of binding by 2 orders of magnitude compared to that of relaxed DNA. The pseudo-first-order rate constant [k psi (sigma)] obeys an exponential function, k psi (sigma) = k psi (lin)e-sigma delta, where delta is a constant of 105 and k psi lin is the rate of PNA binding to linear DNA (sigma = 0). The activation energy [Ea(sigma)] was determined as approximately 93 and approximately 48 kJ mol-1 for PNA binding to linear and supercoiled DNA, respectively. The results are discussed in relation to the possible future use of PNA as an antigene agent and in the framework of DNA "breathing" dynamics.

26] Isolation of avian mitochondrial DNA-less cells

This chapter explains the isolation of Avian mitochondrial DNA-less ( rho ˚) cells. Avian mitochondrial (mt)DNA-less cells have been developed to study the contribution of the mitochondrial genome to the cell phenotype of vertebrates. Rho° cell lines are obtained following long-term exposure of primary chick embryo cells and continuous chicken and quail cells to ethidium bromide, a planar aromatic dye that binds to DNA and RNA by intercalation. Rho° avian cells proliferate in culture with mitochondria devoid of a functional respiratory chain. Rho° avian cells behave phenotypically as Rho° yeast cells obtained following long-term exposure to ethidium bromide. On short-term exposure, large nucleotide sequences are deleted within yeast mtDNA, converting cells to respiration deficient, cytoplasmically inherited petite phenotype mutants. Such mutations are never detected in ethidium bromide-treated vertebrate cells, where mitochondrial DNA (mtDNA) rapidly attains a high negative superhelix density that is reversible on removal of ethidium bromide from the culture medium.

Intramolecular TAT triplex in (dA)58.(dT)58. influence of ions.

Supercoil-stabilized intramolecular triplexes have been described under various conditions in different polypurine.polypyrimidine sequences such as (dG)n.(dC)n and mixed sequences including d(GA)n.d(CT)n while information about the triplexes in (dA)n.(dT)n is scarce. Using osmium tetroxide complexes and diethyl pyrocarbonate as structural probes, we show a pyrimidine.purine.pyrimidine (TAT) triplex in (dA)58.(dT)58 sequence in a supercoiled plasmid pE19. Strong modification of approximately six central thymines and approximately six T's at the 3'-end of the (dT)58 stretch as well as the DEPC modification of the 5'-half of the (dA)58 strand suggested the prevalence of the H-y3 triplex conformer. At native superhelix density, optimum conditions for the triplex formation were close to 1 mM MgCl2, pH 8.5. At room temperature and MgCl2 concentrations below 0.5 and above 5 mM, almost no triplex was formed. It is suggested that the absence of the triplex at higher MgCl2 concentrations is due to the stabilization of the duplex by Mg2+ ions which prevents the duplex opening necessary for the triplex formation. At higher temperatures, favorable for duplex opening (e.g. 55 degrees C), the TAT triplex is formed even in the presence of 10 mM MgCl2. Among Ca2+, Sr2+, Ba2+, Cd2+, Zn2+ and Ni2+, only Ca2+ and Sr2+ yielded a modification pattern similar to that obtained with Mg2+; the modification pattern produced in the presence of Sr2+ was, however, much less intense. In the presence of 1 mM MgCl2, a decrease in pH from 8.5 to 7.7 resulted in a strong decrease of the triplex content. At highly negative superhelix density, the conditions for triplex formation were less stringent, and the triplex was observed even in the absence of MgCl2.