On the chemical yield of base lesions, strand breaks, and clustered damage generated in plasmid DNA by the direct effect of X rays

The purpose of this study was to determine the yield of DNA base damages, deoxyribose damage, and clustered lesions due to the direct effects of ionizing radiation and to compare these with the yield of DNA trapped radicals measured previously in the same pUC18 plasmid. The plasmids were prepared as films hydrated in the range 2.5 < Gamma < 22.5 mol water/mol nucleotide. Single-strand breaks (SSBs) and double-strand breaks (DSBs) were detected by agarose gel electrophoresis. Specific types of base lesions were converted into SSBs and DSBs using the base-excision repair enzymes endonuclease III (Nth) and formamidopyrimidine-DNA glycosylase (Fpg). The yield of base damage detected by this method displayed a strikingly different dependence on the level of hydration (Gamma) compared with that for the yield of DNA trapped radicals; the former decreased by 3.2 times as Gamma was varied from 2.5 to 22.5 and the later increased by 2.4 times over the same range. To explain this divergence, we propose that SSB yields produced in plasmid DNA by the direct effect cannot be analyzed properly with a Poisson process that assumes an average of one strand break per plasmid and neglects the possibility of a single track producing multiple SSBs within a plasmid. The yields of DSBs, on the other hand, are consistent with changes in free radical trapping as a function of hydration. Consequently, the composition of these clusters could be quantified. Deoxyribose damage on each of the two opposing strands occurs with a yield of 3.5 +/- 0.5 nmol/J for fully hydrated pUC18, comparable to the yield of 4.1 +/- 0.9 nmol/J for DSBs derived from opposed damages in which at least one of the sites is a damaged base.     

Study of DNA films by the CD, X-ray and polarization microscopy techniques.

DNA films with psi +/- CD spectra have been investigated. X-ray analysis has shown the sign of the psi spectra to be independent of the secondary structure of DNA. The appearance of the psi spectra is attended by the formation of a characteristic polygonal texture of the cholesteric type in the DNA film.     

Multiplicity of DNA single-strand breaks produced in pUC18 exposed to the direct effects of ionizing radiation

The transition of plasmid DNA from a supercoiled to an open circle conformation, as detected by gel electrophoresis, affords an extraordinarily sensitive method for detecting single-strand breaks (SSBs), one measure of deoxyribose damage. To determine the yield of SSBs, G(ssb), by this method, it is commonly assumed that Poisson statistics apply such that, on average, one SSB occurs per supercoiled plasmid lost. For the direct effect, at a large enough plasmid size, this assumption may be invalid. In this report, the assumption that one SSB occurs per pUC18 plasmid (2686 bp) is tested by measuring free base release (fbr), which is also a measure of deoxyribose damage in films prepared under controlled relative humidity so as to produce known levels of DNA hydration. The level of DNA hydration, Gamma, is expressed in mol water/mol nucleotide. The yield of free base release, G(fbr), was measured by HPLC after exposure of the films to 70 kV X rays and subsequent dissolution in water. It is well known that damage in deoxyribose leads to SSBs and free base release. Based on known mechanisms, there exists a close correspondence between free base release and SSBs, i.e., G(fbr) congruent with G(ssb). Following this assumption, the SSB multiplicity, m(ssb), was determined, where m(ssb) was defined as the mean number of SSBs per supercoiled plasmid lost. The yield of lost supercoil was determined previously (S. Purkayastha et al., J. Phys. Chem. B 110, 26286-26291, 2006). We found that m(ssb) = 1.4 +/- 0.2 at Gamma = 2.5 and m(ssb) = 2.8 +/- 0.5 to 3.1 +/- 0.5 at Gamma = 22.5, indicating that the assumption of one SSB per lost supercoil is not likely to hold for a 2686-bp plasmid exposed to the direct effect. In addition, an increase in G(fbr), upon stepping from Gamma = 2.5 to Gamma = 22.5, was paralleled by an increase in the yield of trapped deoxyribose radicals, G(dRib)(fr), also measured previously. As a consequence, the shortfall between SSBs and trapped radicals, G(diff) = G(ssb) - G(dRib)(fr), remained relatively constant at 90-110 nmol/J. The lack of change between the two extremes of hydration is in keeping with the suggestion that non-radical species, such as doubly oxidized deoxyribose, are responsible for the shortfall.     

Unaltered free base release from d(CGCGCG)2 produced by the direct effect of ionizing radiation at 4 K and room temperature

Unaltered free base release in d(CGCGCG)2 exposed to X rays at 4 K or room temperature was measured by HPLC. Samples were prepared either as films hydrated to a level of Gamma = 2.5 mol water/mol nucleotide or as polycrystalline with Gamma approximately 7.5 mol water/mol nucleotide. X irradiation of films at 4 K, followed by annealing to room temperature, resulted in yields for cytosine and guanine of G(Cyt) = 0.036 +/- 0.001 micromol/J and G(Gua) = 0.090 +/- 0.002 micromol/J. Irradiation of films at room temperature gave similar yields. The yields for polycrystalline d(CGCGCG)2 X-irradiated at room temperature were G(Cyt) = 0.035 +/- 0.005 micromol/J and G(Gua) = 0.077 +/- 0.023 micromol/J. The total free base release yield, G(fbr), was 0.124 +/- 0.008 micromol/J for films and 0.112 +/- 0.028 micromol/J for polycrystalline samples. G(fbr) is believed to be a good estimate of total strand break yield. The yields of total free radicals trapped [G(Sigmafr)] by the d(CGCGCG)2 films at 4 K were measured by EPR. The measured value, G(Sigmafr) = 0.450 +/- 0.005 micromol/J, was used to calculate the yield of trappable sugar radicals, giving G(sugar)(fr) = 0.04-0.07 micromol/J. We found that (1) guanine release exceeded cytosine release by more than twofold, (2) G(sugar)(fr) cannot account for more than half of the free base release, and (3) G(fbr), G(Cyt) and G(Gua) were independent of the sample temperature during irradiation. Finding (1) suggests that base and or sequence influences sugar damage, and finding (2) is consistent with our working hypothesis that an important pathway to strand break formation entails two one-electron oxidations at the same sugar site.     

Auger electron-induced double-strand breaks depend on DNA topology

From a structural perspective, the factors controlling and the mechanisms underlying the toxic effects of ionizing radiation remain elusive. We have studied the consequences of superhelical/torsional stress on the magnitude and mechanism of DSBs induced by low-energy, short-range, high-LET Auger electrons emitted by (125)I, targeted to plasmid DNA by m-[(125)I]iodo-p-ethoxyHoechst 33342 ((125)IEH). DSB yields per (125)I decay for torsionally relaxed nicked (relaxed circular) and linear DNA (1.74+/-0.11 and 1.62+/-0.07, respectively) are approximately threefold higher than that for torsionally strained supercoiled DNA (0.52+/-0.02), despite the same affinity of all forms for (125)IEH. In the presence of DMSO, the DSB yield for the supercoiled form remains unchanged, whereas that for nicked and linear forms decreases to 1.05+/-0.07 and 0.76+/-0.03 per (125)I decay, respectively. DSBs in supercoiled DNA therefore result exclusively from direct mechanisms, and those in nicked and linear DNA, additionally, from hydroxyl radical-mediated indirect effects. Iodine-125 decays produce hydroxyl radicals along the tracks of Auger electrons in small isolated pockets around the decay site. We propose that relaxation of superhelical stress after radical attack could move a single-strand break lesion away from these pockets, thereby preventing further breaks in the complementary strand that could lead to DSBs.     

Release of plasmid DNA from intravascular stents coated with ultrathin multilayered polyelectrolyte films

Materials that permit control over the release of DNA from the surfaces of topologically complex implantable devices, such as intravascular stents, could contribute to the development of new approaches to the localized delivery of DNA. We report the fabrication of ultrathin, multilayered polyelectrolyte films that permit both the immobilization and controlled release of plasmid DNA from the surfaces of stainless steel intravascular stents. Our approach makes use of an aqueous-based, layer-by-layer method for the assembly of nanostructured thin films consisting of alternating layers of plasmid DNA and a hydrolytically degradable polyamine. Characterization of coated stents using scanning electron microscopy (SEM) demonstrated that stents were coated uniformly with an ultrathin film ca. 120 nm thick that adhered conformally to the surfaces of stent struts. These ultrathin films did not crack, peel, or delaminate substantially from the surface after exposure to a range of mechanical challenges representative of those encountered during stent deployment (e.g., balloon expansion). Stents coated with eight bilayers of degradable polyamine and a plasmid encoding enhanced green fluorescent protein (EGFP) sustained the release of DNA into solution for up to four days when incubated in phosphate buffered saline at 37 degrees C, and coated stents were capable of mediating the expression of EGFP in a mammalian cell line without the aid of additional transfection agents. The approach reported here could, with further development, contribute to the development of localized gene-based approaches to the treatment of cardiovascular diseases or related conditions.     

Radiosensitization of DNA by gold nanoparticles irradiated with high-energy electrons

Zheng, Y., Hunting, D. J., Ayotte, P. and Sanche, L. Radiosensitization of DNA by Gold Nanoparticles Irradiated with High-Energy Electrons. Radiat. Res. 168, 19-27 (2008). Thin films of pGEM-3Zf(-) plasmid DNA were bombarded by 60 keV electrons with and without gold nanoparticles. DNA single- and double-strand breaks (SSBs and DSBs) were measured by agarose gel electrophoresis. From transmission electron micrographs, the gold nanoparticles were found to be closely linked to DNA scaffolds, probably as a result of electrostatic binding. The probabilities for formation of SSBs and DSBs from exposure of 1:1 and 2:1 gold nanoparticle:plasmid mixtures to fast electrons increase by a factor of about 2.5 compared to neat DNA samples. For monolayer DNA adsorbed on a thick gold substrate, the damage increases by an order of magnitude. The results suggest that the enhancement of radiosensitivity is due to the production of additional low-energy secondary electrons caused by the increased absorption of ionizing radiation energy by the metal, in the form of gold nanoparticles or of a thick gold substrate. Since short-range low-energy secondary electrons are produced in large amounts by any type of ionizing radiation, and since on average only one gold nanoparticle per DNA molecule is needed to increase damage considerably, targeting the DNA of cancer cells with gold nanoparticles may offer a novel approach that is generally applicable to radiotherapy treatments.     

Mechanisms underlying production of double-strand breaks in plasmid DNA after decay of 125I-Hoechst

Previously, the kinetics of strand break production by (125)I-labeled m-iodo-p-ethoxyHoechst 33342 ((125)IEH) in supercoiled (SC) plasmid DNA had demonstrated that approximately 1 DSB is produced per (125)I decay both in the presence and absence of the hydroxyl radical scavenger DMSO. In these experiments, an (125)IEH:DNA molar ratio of 42:1 was used. We now hypothesize that this DSB yield (but not the SSB yield) may be an overestimate due to subsequent decays occurring in any of the 41 (125)IEH molecules still bound to nicked (N) DNA. To test our hypothesis, (125)IEH was incubated with SC pUC19 plasmids ((125)IEH:DNA ratio of approximately 3:1) and the SSB and DSB yields were quantified after the decay of (125)I. As predicted, the number of DSBs produced per (125)I decay is one-half that reported previously ( approximately 0.5 compared to approximately 1, +/- DMSO) whereas the number of SSBs ( approximately 3/(125)I decay) is similar to that obtained previously ( approximately 90% are generated by OH radicals). Direct visualization by atomic force microscopy confirms formation of L and N DNA after (125)IEH decays in SC DNA and supports the strand break yields reported. These findings indicate that although SSB production is independent of the number of (125)IEH bound to DNA, the DSB yield can be augmented erroneously by (125)I decays occurring in N DNA. Further analysis indicates that 17% of SSBs and 100% of DSBs take place within the plasmid molecule in which an (125)IEH molecule decays, whereas 83% of SSBs are formed in neighboring plasmid DNA molecules.     

Reactive thin polymer films as platforms for the immobilization of biomolecules

Spin-coated thin films of poly(N-hydroxysuccinimidyl methacrylate) (PNHSMA) on oxidized silicon and gold surfaces were investigated as reactive layers for obtaining platforms for biomolecule immobilization with high molecular loading. The surface reactivity of PNHSMA films in coupling reactions with various primary amines, including amine-terminated poly(ethylene glycol) (PEG-NH2) and fluoresceinamine, was determined by Fourier transform infrared (FTIR) spectroscopy, X-ray photoelectron spectroscopy (XPS), fluorescence microscopy, and ellipsometry measurements, respectively. The rate constants of PEG-NH2 attachment on the PNHSMA films were found to be significantly increased compared to the coupling on self-assembled monolayers (SAMs) of 11,11'-dithiobis(N-hydroxysuccinimidylundecanoate) (NHS-C10) on gold under the same conditions. More significantly, the PEG loading observed was about 3 times higher for the polymer thin films. These data indicate that the coupling reactions are not limited to the very surface of the polymer films, but proceed into the near-surface regions of the films. PNHSMA films were shown to be stable in contact with aqueous buffer; the swelling analysis, as performed by atomic force microscopy (AFM), indicated a film thickness independent swelling of approximately 2 nm. An increased loading was also observed by surface plasmon resonance for the covalent immobilization of amino-functionalized probe DNA. Hybridization of fluorescently labeled target DNA was successfully detected by fluorescence microscopy and surface plasmon resonance enhanced fluorescence spectroscopy (SPFS), thereby demonstrating that thin films of PNHSMA comprise an attractive and simple platform for the immobilization of biomolecules with high densities.     

Morphological studies of oligodeoxyribonucleotides probes covalently immobilized at polystyrene modified surfaces

The immobilization of short ss-DNA (18- and 36-mer) and their hybridization were studied at gold and glassy carbon substrates modified with low molecular weight (approximately 12, 18 and 24 kg/mol) polystyrene thin films. Amino-modified DNA was attached to the surface by reaction with succinimide ester groups bound to the polystyrenes. A ferrocene modified DNA target was used to confirm the probe-target hybridization. Atomic force microscopy studies showed significant morphological changes after probe immobilization and hybridization compared to the featureless structure of the polystyrene film. Single-stranded DNA samples had a globular morphology with an average density of 3.8 and 2.2 (x 10(11)) globules/cm2 for the 18- and 36-mer, respectively. The formation of a porous structure with a 2.0 and 1.0 (x10(11)) average pore density corresponding to the 18- and 36-mer was observed after hybridization. A surface composition analysis was done by X-ray photoelectron spectroscopy to confirm and support the images interpretation. Ferrocene oxidation (+323 mV/18-mer, +367 mV/36-mer, versus Ag/AgCl) proved the presence of ds-DNA at the modified surfaces.     

Radial displacement of myosin cross-bridges in mouse myocardium due to ablation of myosin binding protein-C

Myosin binding protein-C (cMyBP-C) is a thick filament accessory protein, which in cardiac muscle functions to regulate the kinetics of cross-bridge interaction with actin; however, the underlying mechanism is not yet understood. To explore the structural basis for cMyBP-C function, we used synchrotron low-angle X-ray diffraction to measure interfilament lattice spacing and the equatorial intensity ratio, I(11)/I(10), in skinned myocardial preparations isolated from wild-type (WT) and cMyBP-C null (cMyBP-C(-/-)). In relaxed myocardium, ablation of cMyBP-C appeared to result in radial displacement of cross-bridges away from the thick filaments, as there was a significant increase ( approximately 30%) in the I(11)/I(10) ratio for cMyBP-C(-/-) (0.37+/-0.03) myocardium as compared to WT (0.28+/-0.01). While lattice spacing tended to be greater in cMyBP-C(-/-) myocardium (44.18+/-0.68 nm) when compared to WT (42.95+/-0.43 nm), the difference was not statistically significant. Furthermore, liquid-like disorder in the myofilament lattice was significantly greater ( approximately 40% greater) in cMyBP-C(-/-) myocardium as compared to WT. These results are consistent with our working hypothesis that cMyBP-C normally acts to tether myosin cross-bridges nearer to the thick filament backbone, thereby reducing the likelihood of cross-bridge binding to actin and limiting cooperative activation of the thin filament.     

DNA interduplex crosslinks induced by Al(Kalpha) X rays under vacuum

Dry pGEM-3Zf(-) plasmid DNA was exposed to Al(kalpha) X rays (1.5 keV) for various times in an ultra-high vacuum chamber with mean absorbed dose rates ranging from 1.8 to 41.7 Gy s(-1). The different forms of plasmid DNA were separated by neutral agarose gel electrophoresis and quantified by staining and laser scanning. In addition to the bands for supercoiled, nicked circular, linear and concatameric forms of plasmid DNA, two additional bands were observed in X-irradiated samples; these migrated at rates similar to those for 8-kb and >10-kb linear double-stranded DNA. Digestion of irradiated DNA with the restriction enzymes EcoR1 and PvuI suggested that the two slowly migrating bands were interduplex crosslinked DNA. Alkaline agarose gel electrophoresis of irradiated DNA digested with EcoR1 confirmed that the interduplex crosslink was covalent. Exposure-response curves were determined for the formation of nicked circular, linear and interduplex crosslinked DNA as well as for the loss of supercoiled and concatameric DNA. Formation and loss of these species were independent of absorbed dose rate over a 20-fold range. The G values for DNA single-strand breaks, double-strand breaks and crosslinks were determined to be 62 +/- 6, 5.6 +/- 0.6 and 16 +/- 4 nmol J(-1), respectively. The formation of DNA interduplex crosslinks appears to be due to single event. The mechanism responsible for the formation of DNA interduplex crosslinks is discussed with emphasis on its implications in vivo.     

A high-power vircator operating as an X-ray bremsstrahlung generator

Avircator capable of generating high-power X-ray pulses due to the multiple transitions of electrons through a thin anode foil transparent to X radiation has been created and put into operation for the first time. The vircator is created on the basis of a direct-action electron accelerator supplied from an inductive energy storage operating with a plasma opening switch. Self-consistent two-dimensional simulations of the electron beam dynamics in the vircator chamber are performed, and the spectra of the generated microwave radiation are determined. Self-consistent one-dimensional simulations of the beam dynamics with allowance for electron scattering in the foil were also carried out, and the X-ray bremsstrahlung spectra were measured. Results are presented from the first experiments on the generation of X-ray bremsstrahlung in vircators with thin (10 μm) and thick (100 μm) tantalum anode foils. For a thin foil, the X-ray (E _γ>30 keV) dose is eight times as high as that for a thick foil and the average photon energy is 30 keV (against 80 keV for a thick foil). __________ Translated from Fizika Plazmy, Vol. 30, No. 9, 2004, pp. 828–834. Original Russian Text Copyright ￠ 2004 by Selemir, Dubinov, Ryaslov, Kargin, Efimova, Loyko.     

Flexible chitin films: structural studies

Chitin gels were transformed into thin, flexible chitin films with minimal dimensional shrinkage and maximum flexibility and thickness in the range of 25-80 microm by a cold-press process. Solvent residue was removed by heating the films at 50 degrees C for 12 h, followed by rinsing in 95% ethanol. The crystallinity and mechanical properties of the flexible chitin films were found to be a function of the amount of shrinkage from the gel to the final film that was obtained. For 28-microm thick films with 30% shrinkage, transparency of up to 90% was found. X-ray diffractometry (XRD) showed that the number of diffraction peaks appearing at 2theta;=23 degrees and 2theta;=27 degrees became increasingly sharper with shrinkage. Topographical information obtained from scanning electron microscopy (SEM) and atomic force microscopy (AFM) attributed the structural morphology of the films to the formation of sub-microscopic micelles. Scanning transmission electron microscopy (STEM) showed that shrinkage resulted in coarser microstructure, affecting tensile properties, where the ductility and toughness were proportional to the amount of shrinkage. These flexible chitin films have potential as wound dressing materials.     

Electron microscopic study of conjugative plasmids from serologically typed E. coli AP1]

The plasmid DNAs isolated from E. coli AP1 were studied by electron microscopy. Two plasmid DNA forms (FB1-1 and FB1--2) with the mol wt of 35.9 +/- 0.5 x x 10(6) and 51.5 +/- 0.6 x 10(6) daltons, respectively, were revealed.     

Inkjet‐Printed Micrometer‐Thick Perovskite Solar Cells with Large Columnar Grains

Transferring the high power conversion efficiencies (PCEs) of spin‐coated perovskite solar cells (PSCs) on the laboratory scale to large‐area photovoltaic modules requires a significant advance in scalable fabrication methods. Digital inkjet printing promises scalable, material, and cost‐efficient deposition of perovskite thin films on a wide range of substrates and in arbitrary shapes. In this work, high‐quality inkjet‐printed triple‐cation (methylammonium, formamidinium, and cesium) perovskite layers with exceptional thicknesses of >1 µm are demonstrated, enabling unprecedentedly high PCEs > 21% and stabilized power output efficiencies > 18% for inkjet‐printed PSCs. In‐depth characterization shows that the thick inkjet‐printed perovskite thin films deposited using the process developed herein exhibit a columnar crystal structure, free of horizontal grain boundaries, which extend over the entire thickness. A thin film thickness of around 1.5 µm is determined as optimal for PSC for this process. Up to this layer thickness X‐ray photoemission spectroscopy analysis confirms the expected stoichiometric perovskite composition at the surface and shows strong deviations and inhomogeneities for thicker thin films. The micrometer‐thick perovskite thin films exhibit remarkably long charge carrier lifetimes, highlighting their excellent optoelectronic characteristics. They are particularly promising for next‐generation inkjet‐printed perovskite solar cells, photodetectors, and X‐ray detectors.     

O2 transfer kinetics in a whole blood unicellular thin layer

A planar monocellular layer of whole blood (WB) sandwiched between two Gore-Tex membranes is used to study O2 uptake and release kinetics at 37 degrees C. Gore-Tex, a highly gas-permeable open mesh of Teflon fibrils (78% porosity, 0.2-microns pore size, 75-microns thick), constrains WB to form a thin film without imposing an appreciable gas diffusion barrier. WB layer thickness, measured by isotope dilution, is 1.7 +/- 0.2 microns. WB films are mounted between fiber optics in a gas flow tube for dual-wavelength (536/558 nm) oxyhemoglobin saturation measurements after a step change in PO2. For isocapnic (6% CO2) step changes in PO2 between 0 and 104 Torr, WB O2 uptake half time is 10.4 +/- 0.9 ms; WB O2 release half time is 20.6 +/- 2.4 ms. Half-time values are half of those previously reported. The thin-layer method reduces erythrocyte diffusion boundary layer error and thereby offers an attractive alternative to classical rapid fluid-mixing techniques.     

Adsorption of plasmid DNA onto N,N'- (dimethylamino)ethyl-methacrylate graft-polymerized poly-L-lactic acid film surface for promotion of in-situ gene delivery

The surface of biodegradable poly-L-lactic acid (PLLA) film was modified with N,N'-(dimethylamino)ethyl-methacrylate (DMAEMA) via UV-induced graft copolymerization, and plasmid DNA molecules were adsorbed onto the surface of modified PLLA film by electrostatic interactions with cationic DMAEMA polymer. We characterized the structure of the modified PLLA film surface by Fourier transform infrared attenuated total reflection (FTIR-ATR) spectroscopy and X-ray photoelectron spectroscopy (XPS). The weight-average molecular weight (Mw) of grafted DMAEMA polymer chains was estimated from the elution time of gel filtration chromatography. C.I. Acid Orange 7 dyeing results indicated that graft density of DMAEMA on PLLA film increased with the UV irradiation time and then reached a saturated value. DNA adsorption density was proportioned to graft density of DMAEMA. Mouse fibroblast L929 cell line was cultured on modified PLLA films, and cell viability and gene transfection efficiency were monitored after 2 days culture. It was found that the DMAEMA grafted PLLA film had obvious cytotoxicity to the cells. On the contrary, cytotoxicity of the surface was highly decreased after adsorption with plasmid DNA. This DNA adsorbed DMAEMA modified PLLA showed the ability to deliver DNA into mammalian cells cultured on the surface with high-transfection efficiency at a low DNA amount. The present results suggest that the DMAEMA grafted PLLA has potentiality to be used as a safe and effective gene delivery system in gene-activated materials.     

Analysis of three overexpression systems for VanX, the Zinc(II) dipeptidase required for high-level vancomycin resistance in bacteria

The gene from Enterococcus faecilis encoding the dipeptidase VanX was subcloned into overexpression vectors pET-5b, pET-27b, and IMPACT-T7, and VanX was overexpressed in BL21(DE3) pLysS Escherichia coli. The pET-5b-vanx overexpression plasmid produces VanX at approximately 12 mg/L under optimum conditions. VanX produced from this overexpression system exists primarily as a dimer in solution, binds ca. 1 Zn(II) ion per monomer, and exhibits K(m) and k(cat) values of 500 +/- 40 microM and 0.074 +/- 0.001 s(-1), respectively, when l-alanine-p-nitroanilide is used as substrate. The IMPACT-T7-vanx overexpression plasmid produces a VanX-fusion protein with a chitin-binding domain that allows for purification of the fusion construct with a chitin column. Cleavage of the fusion protein is completed by an on-column chemical cleavage, resulting in approximately 10 mg/L of purified VanX. VanX produced from this system is identical to that produced from the pET-5b system, except the CD spectrum of the IMPACT-T7-produced VanX suggests a small change in secondary structure. This change in secondary structure does not affect any of the kinetic or metal-binding properties of the enzyme. The pET-27b-vanx overexpression plasmid produces and secretes VanX into the growth medium; this system allows for 20 mg of VanX to be isolated per liter of growth medium. The pET-27b-produced VanX is identical to that produced from pET-5b.     

Plasmid DNA breakage by decay of DNA-associated Auger electron emitters: approaches to analysis of experimental data

Plasmid DNA is a popular substrate for the assay of DNA strand breakage by a variety of agents. The use of the plasmid assay relies on the assumption that individual damaging events occur at random, which allows the application of Poisson statistics. This assumption is not valid in the case of damage arising from decay of DNA-associated Auger electron emitters, since a single decay event can generate a few breaks in the same DNA strand, which is indistinguishable from a single break in the assay. The consequent analytical difficulties are overcome by considering relaxation events rather than single-strand breaks, and linearization events rather than double-strand breaks. A further consideration is that apart from damage at the site of DNA-associated decay, which is the principal interest of the analysis, some DNA damage also arises from the radiation field created by all decay events. These two components of damage are referred to as internal and external breakage, respectively, and they can be separated in the analysis since their contribution depends on the experimental conditions. The DNA-binding ligand Hoechst 33258 labeled with 125I was used in our experiments to study breakage in pBR322 plasmid DNA arising from the decay of this Auger electron emitter. The values obtained for the efficiency (per decay) of plasmid relaxation and linearization by the 125I-labeled ligand were 0.090 +/- 0.035 and 0.82 +/- 0.04, respectively. When dimethylsulfoxide was included as a radical scavenger, the efficiency values for relaxation and linearization were 0.15 +/- 0.02 and 0.65 +/- 0.05, respectively.