Monte Carlo simulation of strand-break induction on plasmid DNA in aqueous solution by monoenergetic electrons

The radiation-induced process of strand breaks on pBR322 plasmid DNA in aqueous solution for different energy electrons was studied by Monte Carlo simulation. Assumptions of induction mechanisms of single- and double-strand breaks (SSBs and DSBs) used in the simulation are that SSB is induced by OH or H reaction with DNA and that DSB is induced by two SSBs on the opposite strands within 10 bp. Dose-response relationships of SSBs and DSBs were demonstrated for monoenergetic electrons of 100 eV, 10 keV, 1 keV and 1 MeV, and the yields of SSB and DSB were calculated. The dose-response relationships of SSBs and DSBs can be fitted by linear and linear-quadratic functions, respectively. The ratio of quadratic to linear components of DSB induction changes due to the electron energy. A high contribution of the linear component is observed for 1 keV electrons in the dose range below 160 Gy. The yields of SSBs and DSBs for all examined electron energies lie well within the experimental data when the probability of strand-break induction by OH and H is assumed to be around 0.1-0.2. The yield of SSBs has a minimum at 1 keV, while the yield of DSBs has a maximum at 1 keV in the examined energies. The strand breaks are formed most densely for 1 keV electrons.     

Calculation of radiation-induced DNA damage from photons and tritium beta-particles

Radiation-induced damage in nucleosomal DNA was modelled by Monte Carlo means. An atomistic representation of DNA with a first hydration shell was used. DNA single- and double-strand break (SSB and DSB) yields were calculated for ¹³⁷Cs photons, x-rays and tritium beta-particles. Monte Carlo-generated electron tracks for liquid water were used to model energy deposition. Chemical evolution of a track and interactions between species and DNA following water radiolysis were modelled in an encounter-controlled manner. The effects of varying the scavenging capacity of the environment, the extent of DNA protection by histones and the setting of a threshold for direct energy depositions on DNA break yields were all systematically studied. DSB complexity was assessed in terms of DNA breaks and base damage accompanying a DSB. Model parameters were adjusted to make predictions consistent with experimental data on DSB yields and yield modification by a variety of factors including changing DNA conformation and incorporation of scavengers. An embedded model of nucleosomal DNA by histones was required to explain experimentally observed modification of DSB yield by removal of bound histones. Complex DSB, defined as DSB accompanied by an additional strand breakage, exhibited high association with base damage. It is shown that hydroxyl radical interactions with bases are a major contributor to DSB complexity. On average there were 1.15 and 2.69 OH-base interactions accompanying simple and complex DSB, respectively for ¹³⁷Cs. Over 80% of complex DSB had at least one OH-base interaction associated with a DNA break. Received: 21 March 2000 / Accepted: 27 October 2000     

Mechanism of cell killing after ionizing radiation by a dominant negative DNA polymerase beta

Several types of DNA lesion are induced after ionizing irradiation (IR) of which double strand breaks (DSBs) are expected to be the most lethal, although single strand breaks (SSBs) and DNA base damages are quantitatively in the majority. Proteins of the base excision repair (BER) pathway repair these numerous lesions. DNA polymerase beta has been identified as a crucial enzyme in BER and SSB repair (SSBR). We showed previously that inhibition of BER/SSBR by expressing a dominant negative DNA polymerase beta (polβDN) resulted in radiosensitization. We hypothesized increased kill to result from DSBs arising from unrepaired SSBs and BER intermediates. We find here higher numbers of IR-induced chromosome aberrations in polβDN expressing cells, confirming increased DSB formation. These aberrations did not result from changes in DSB induction or repair of the majority of lesions. SSB conversion to DSBs has been shown to occur during replication. We observed an increased induction of chromatid aberrations in polβDN expressing cells after IR, suggesting such a replication-dependence of secondary DSB formation. We also observed a pronounced increase of chromosomal deletions, the most likely cause of the increased kill. After H₂O₂ treatment, polβDN expression only resulted in increased chromatid (not chromosome) aberrations. Together with the lack of sensitization to H₂O₂, these data further suggest that the additional secondarily induced lethal DSBs resulted from repair attempts at complex clustered damage sites, unique to IR. Surprisingly, the polβDN induced increase in residual γH2AX foci number was unexpectedly low compared with the radiosensitization or induction of aberrations. Our data thus demonstrate the formation of secondary DSBs that are reflected by increased kill but not by residual γH2AX foci, indicating an escape from γH2AX-mediated DSB repair. In addition, we show that in the polβDN expressing cells secondary DSBs arise in a radiation-specific and partly replication-dependent manner.     

Measurement of complex DNA damage induction and repair in human cellular systems after exposure to ionizing radiations of varying linear energy transfer (LET)

Abstract

Detrimental effects of ionizing radiation (IR) are correlated to the varying efficiency of IR to induce complex DNA damage. A double strand break (DSB) can be considered the simpler form of complex DNA damage. These types of damage can consist of DSBs, single strand breaks (SSBs) and/or non-DSB lesions such as base damages and apurinic/apyrimidinic (AP; abasic) sites in different combinations. Enthralling theoretical (Monte Carlo simulations) and experimental evidence suggests an increase in the complexity of DNA damage and therefore repair resistance with linear energy transfer (LET). In this study, we have measured the induction and processing of DSB and non-DSB oxidative clusters using adaptations of immunofluorescence. Specifically, we applied foci colocalization approaches as the most current methodologies for the in situ detection of clustered DNA lesions in a variety of human normal (FEP18-11-T1) and cancerous cell lines of varying repair efficiency (MCF7, HepG2, A549, MO59K/J) and radiation qualities of increasing LET, that is γ-, X-rays 0.3–1?keV/μm, α-particles 116?keV/μm and ³⁶Ar ions 270?keV/μm. Using γ-H2AX or 53BP1 foci staining as DSB probes, we calculated a DSB apparent rate of 5–16 DSBs/cell/Gy decreasing with LET. A similar trend was measured for non-DSB oxidized base lesions detected using antibodies against the human repair enzymes 8-oxoguanine-DNA glycosylase (OGG1) or AP endonuclease (APE1), that is damage foci as probes for oxidized purines or abasic sites, respectively. In addition, using colocalization parameters previously introduced by our groups, we detected an increasing clustering of damage for DSBs and non-DSBs. We also make correlations of damage complexity with the repair efficiency of each cell line and we discuss the biological importance of these new findings with regard to the severity of IR due to the complex nature of its DNA damage.     

Radiation induced DNA DSBs: Contribution from stalled replication forks?

When cells are exposed to radiation serious lesions are introduced into the DNA including double strand breaks (DSBs), single strand breaks (SSBs), base modifications and clustered damage sites (a specific feature of ionizing radiation induced DNA damage). Radiation induced DNA damage has the potential to initiate events that can lead ultimately to mutations and the onset of cancer and therefore understanding the cellular responses to DNA lesions is of particular importance. Using γH2AX as a marker for DSB formation and RAD51 as a marker of homologous recombination (HR) which is recruited in the processing of frank DSBs or DSBs arising from stalled replication forks, we have investigated the contribution of SSBs and non-DSB DNA damage to the induction of DSBs in mammalian cells by ionizing radiation during the cell cycle. V79-4 cells and human HF19 fibroblast cells have been either irradiated with 0–20 Gy of γ radiation or, for comparison, treated with a low concentration of hydrogen peroxide, which is known to induce SSBs but not DSBs. Inhibition of the repair of oxidative DNA lesions by poly(ADP ribose) polymerase (PARP) inhibitor leads to an increase in radiation induced γH2AX and RAD51 foci which we propose is due to these lesions colliding with replication forks forming replication induced DSBs. It was confirmed that DSBs are not induced in G₁ phase cells by treatment with hydrogen peroxide but treatment does lead to DSB induction, specifically in S phase cells. We therefore suggest that radiation induced SSBs and non-DSB DNA damage contribute to the formation of replication induced DSBs, detected as RAD51 foci.     

Repair of HZE-particle-induced DNA double-strand breaks in normal human fibroblasts

DNA damage generated by high-energy and high-Z (HZE) particles is more skewed toward multiply damaged sites or clustered DNA damage than damage induced by low-linear energy transfer (LET) X and gamma rays. Clustered DNA damage includes abasic sites, base damages and single- (SSBs) and double-strand breaks (DSBs). This complex DNA damage is difficult to repair and may require coordinated recruitment of multiple DNA repair factors. As a consequence of the production of irreparable clustered lesions, a greater biological effectiveness is observed for HZE-particle radiation than for low-LET radiation. To understand how the inability of cells to rejoin DSBs contributes to the greater biological effectiveness of HZE particles, the kinetics of DSB rejoining and cell survival after exposure of normal human skin fibroblasts to a spectrum of HZE particles was examined. Using gamma-H2AX as a surrogate marker for DSB formation and rejoining, the ability of cells to rejoin DSBs was found to decrease with increasing Z; specifically, iron-ion-induced DSBs were repaired at a rate similar to those induced by silicon ions, oxygen ions and gamma radiation, but a larger fraction of iron-ion-induced damage was irreparable. Furthermore, both DNA-PKcs (DSB repair factor) and 53BP1 (DSB sensing protein) co-localized with gamma-H2AX along the track of dense ionization produced by iron and silicon ions and their focus dissolution kinetics was similar to that of gamma-H2AX. Spatial co-localization analysis showed that unlike gamma-H2AX and 53BP1, phosphorylated DNA-PKcs was localized only at very specific regions, presumably representing the sites of DSBs within the tracks. Examination of cell survival by clonogenic assay indicated that cell killing was greater for iron ions than for silicon and oxygen ions and gamma rays. Collectively, these data demonstrate that the inability of cells to rejoin DSBs within clustered DNA lesions likely contributes to the greater biological effectiveness of HZE particles.     

Age and gender effects on DNA strand break repair in peripheral blood mononuclear cells

Exogenous and endogenous damage to DNA is constantly challenging the stability of our genome. This DNA damage increase the frequency of errors in DNA replication, thus causing point mutations or chromosomal rearrangements and has been implicated in aging, cancer, and neurodegenerative diseases. Therefore, efficient DNA repair is vital for the maintenance of genome stability. The general notion has been that DNA repair capacity decreases with age although there are conflicting results. Here, we focused on potential age‐associated changes in DNA damage response and the capacities of repairing DNA single‐strand breaks (SSBs) and double‐strand breaks (DSBs) in human peripheral blood mononuclear cells (PBMCs). Of these lesions, DSBs are the least frequent but the most dangerous for cells. We have measured the level of endogenous SSBs, SSB repair capacity, γ‐H2AX response, and DSB repair capacity in a study population consisting of 216 individuals from a population‐based sample of twins aged 40–77 years. Age in this range did not seem to have any effect on the SSB parameters. However, γ‐H2AX response and DSB repair capacity decreased with increasing age, although the associations did not reach statistical significance after adjustment for batch effect across multiple experiments. No gender differences were observed for any of the parameters analyzed. Our findings suggest that in PBMCs, the repair of SSBs is maintained until old age, whereas the response to and the repair of DSBs decrease.     

Repair of radiation-induced heat-labile sites is independent of DNA-PKcs, XRCC1 and PARP

Ionizing radiation induces a variety of different DNA lesions; in addition to the most critical DNA damage, the DSB, numerous base alterations, SSBs and other modifications of the DNA double-helix are formed. When several non-DSB lesions are clustered within a short distance along DNA, or close to a DSB, they may interfere with the repair of DSBs and affect the measurement of DSB induction and repair. We have shown previously that a substantial fraction of DSBs measured by pulsed-field gel electrophoresis (PFGE) are in fact due to heat-labile sites within clustered lesions, thus reflecting an artifact of preparation of genomic DNA at elevated temperature. To further characterize the influence of heat-labile sites on DSB induction and repair, cells of four human cell lines (GM5758, GM7166, M059K, U-1810) with apparently normal DSB rejoining were tested for biphasic rejoining after gamma irradiation. When heat-released DSBs were excluded from the measurements, the fraction of fast rejoining decreased to less than 50% of the total. However, the half-times of the fast (t(1/2) = 7-8 min) and slow (t(1/2) = 2.5 h) DSB rejoining were not changed significantly. At t = 0, the heat-released DSBs accounted for almost 40% of the DSBs, corresponding to 10 extra DSBs per cell per Gy in the initial DSB yield. These heat-released DSBs were repaired within 60-90 min in all cells tested, including M059K cells treated with wortmannin and DNA-PKcs-defective M059J cells. Furthermore, cells lacking XRCC1 or poly(ADP-ribose) polymerase 1 (PARP1) rejoined both total DSBs and heat-released DSBs similarly to normal cells. In summary, the presence of heat-labile sites has a substantial impact on DSB induction and DSB rejoining rates measured by pulsed-field gel electrophoresis, and heat-labile sites repair is independent of DNA-PKcs, XRCC1 and PARP.     

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.     

Influence of radiation quality on the yield of DNA strand breaks in SV40 DNA irradiated in solution.

Using highly energetic particles to irradiate plasmid DNA in aerobic aqueous solution, we have compiled an extensive database on how yields of DNA single- and double-strand breaks (SSBs and DSBs) vary with radiation quality. This study was performed in a low-scavenging buffer system and covers a wide range of ion species (helium to uranium) and LETs (5 to 16,000 keV/microm). For LETs up to around 40 keV/microm for SSBs and 400 keV/microm for DSBs, the total energy deposition determines cross section. At higher LET, cross sections level off and individual plateaus for particles of different atomic numbers are observed. For each ion species this is more pronounced and occurs at lower LET for SSBs than for DSBs, leading to an increase in the DSB:SSB ratio from 1:70 for X rays to 1:6 at 500 keV/microm. At this LET, the influence of track structure becomes evident, with high local concentrations of ionization events favoring the formation of DSBs and also intratrack recombination reactions. For lower-energy ions, a saturation in production of measurable DSBs is apparent, due to correlated lesion induction within densely ionizing particle tracks. For very heavy low-energy ions, both SSB and DSB cross sections decrease with particle velocity at nearly constant LET, forming individual hooked curves when plotted as a function of LET.     

Induction and rejoining of gamma-ray-induced DNA single- and double-strand breaks in Chinese hamster AA8 cells and in two radiosensitive clones

The induction and rejoining of gamma-ray-induced DNA strand breaks were measured in a Chinese hamster ovary cell line, AA8, and in two radiosensitive clones (EM9 and NM2) derived from it. The kinetics of recovery from sublethal damage (SLD) and potentially lethal damage (PLD) has previously been characterized in each of these lines [vanAnkeren et al., Radiat. Res., 115, 223-237 (1988)]. No significant differences were observed among the cell lines in the yields of either DNA single-strand breaks (SSBs) or double-strand breaks (DSBs) as assayed by filter elution. Data for SSB rejoining in AA8 and NM2 cells irradiated with 7.5 Gy were fit by a biexponential process (t1/2 values of approximately 4 and 80 min). In comparison, SSB rejoining in EM9 cells was initially slower (t1/2 = 10 min) and a higher level of SSBs was unrejoined 6 h after irradiation. DSB rejoining in AA8 cells assayed at pH 9.6 was also biphasic (t1/2 values of 15 and 93 min), although when assayed at pH 7.0, most (approximately 80%) of the damage was rejoined at a constant rate (t1/2 = 45 min) during the first 2 h. EM9 cells exhibited a slower initial rate of DSB rejoining when assayed at pH 9.6 but showed no difference compared with AA8 cells in DSB rejoining when assayed at pH 7.0. These results indicate that radiosensitive EM9 cells, whose kinetics of recovery from SLD and PLD was the same as that of AA8 cells, have a defect in the fast phase of SSB rejoining but no measurable defect in DSB rejoining. Conversely, NM2 cells, which displayed a reduced shoulder width on their survival curve and decreased recovery from SLD, had no demonstrable defects in the rate or extent of rejoining of DSBs or SSBs. When compared with the SLD and PLD data reported previously, these results suggest that there is no direct correlation between either of these recovery processes and the rejoining of SSBs or DSBs as assayed here.     

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.     

Activation of ataxia telangiectasia mutated by DNA strand break-inducing agents correlates closely with the number of DNA double strand breaks

The protein kinase ataxia telangiectasia mutated (ATM) is activated when cells are exposed to ionizing radiation (IR). It has been assumed that ATM is specifically activated by the few induced DNA double strand breaks (DSBs), although little direct evidence for this assumption has been presented. DSBs constitute only a few percent of the IR-induced DNA damage, whereas the more frequent single strand DNA breaks (SSBs) and base damage account for over 98% of the overall DNA damage. It is therefore unclear whether DSBs are the only IR-induced DNA lesions that activate ATM. To test directly whether or not DSBs are responsible for ATM activation, we exposed cells to drugs and radiation that produce different numbers of DSBs and SSBs. We determined the resulting ATM activation by measuring the amount of phosphorylated Chk2 and the numbers of SSBs and DSBs in the same cells after short incubation periods. We found a strong correlation between the number of DSBs and ATM activation but no correlation with the number of SSBs. In fact, hydrogen peroxide, which, similar to IR, induces DNA damage through hydroxyl radicals but fails to induce DSBs, did not activate ATM. In contrast, we found that calicheamicin-induced strand breaks activated ATM more efficiently than IR and that ATM activation correlated with the relative DSB induction by these agents. Our data indicate that ATM is specifically activated by IR-induced DSBs, with little or no contribution from SSBs and other types of DNA damage. These findings have implications for how ATM might recognize DSBs in cells.     

Modelling the probability distribution of the number of DNA double-strand breaks due to sporadic alkylation of nucleotide bases

Metabolites and certain chemical agents (for example methyl methanesulfonate) can induce nucleotide bases on chromosomal strands to become alkylated. These alkylated sites have the potential to become single-strand chromosomal breaks, a form of DNA damage, if they are exposed to a sufficient temperature in vitro. It has been proposed that a single-strand break (SSB) sufficiently close to another SSB on the opposite chromosomal strand will form a double-strand break (DSB). DNA repair mechanisms are less able to repair DSBs compared to SSBs. Because of the complex three-dimensional structure of DNA, some chromosomal regions are more susceptible to alkylation than others. A question of interest is therefore whether these alkylated bases are randomly distributed or tend to be clustered. Pulsed-field gel electrophoresis allows the number of DNA fragments (and hence the number of DSBs) to be observed directly. The randomness of alkylation events can therefore be tested using the standard statistical hypothesis-testing framework. Under the null hypothesis, that the SSBs are randomly distributed on each of the strands, we can calculate the probability of observing a number of DSBs at least as large as that observed and hence the associated p-value. Previously, the probability distribution of the number of DSBs has been determined by Monte Carlo simulations; when considering the whole genome this can be very time consuming. In this paper, we theoretically derive an approximation to the distribution enabling appropriate probabilities to be calculated quickly. Based on previous findings we assume that the number of breaks on each strand is small compared to the number of nucleotide bases. We show that our method can give the correct probability distribution when alkylation events are relatively rare, discuss how rare these events have to be and suggest potential extensions to the model when a greater proportion of bases are alkylated.     

Elaboration of cellular DNA breaks by hydroperoxides.

Cellular damage produced by ionizing radiation and peroxides, hydrogen peroxide (HOOH) and the organic peroxides tert-butyl (tBuOOH) or cumene hydroperoxide (CuOOH) were compared. DNA breaks, toxicity, malondialdehyde production, and the rate of peroxide disappearance were measured in a human adenocarcinoma cell line (A549). The alkaline and neutral filter elution assays were used to quantitate the kinetics of single and double strand break formation and repair (SSB and DSB), respectively. Peroxides, at 0.01-1.0 mM, produce multiphasic dose response curves for both toxicity and DNA SSBs. Radiation, 1-6 Gy, produced a shouldered survival curve, and both DNA SSB and DSBs produced in cells x-rayed on ice were nearly linear with dose. The peroxides produced more SSBs than radiation at equitoxic doses. X-ray induced DNA single strand breaks were rejoined rapidly by cells at 37 degrees C with approximately 80% of initial damage repaired in 20 min. Peroxide induced SSBs were maximal after 15 min at 37 degrees C. Rejoining proceeded thereafter, but at a rate less than for x-ray induced strand breaks. Significant DNA DSBs could not be achieved by peroxides even at concentrations 50-fold higher than required to produce SSBs. HOOH treatment of DNA on filters following cell lysis and proteolysis produced SSBs. CuOOH and tBuOOH produced no SSBs in lysed cell DNA. None of the peroxides produced DSBs when incubated with lysed cell DNA. Malondialdehyde was released from cells incubated with organic hydroperoxides, but not HOOH, nor up to 40 Gy of x-rays. HOOH was metabolized three times faster than the organic peroxides. The overall results demonstrate the necessity for a metabolically active cell environment to elaborate maximal DNA strand breaks and cell death at hydroperoxide concentrations of 10(-4) or greater, but prevent strand breaks and stimulate cell growth at 10(-5) M.     

Apex1 can cleave complex clustered DNA lesions in cells

Current data indicate that clustered DNA damage generated by ionizing radiation contains 2–5 damages within 20 bps. The complexity of clustered damage is also believed to increase as the linear energy transfer of the radiation increases. Complex lesions are therefore biologically relevant especially with the use of carbon ion beam therapy to treat cancer. Since two closely opposed AP site analogs (furans) are converted to a double strand break (DSB) in cells, we hypothesized that breakage could be compromised by increasing the complexity of the cluster. We have examined the repair of clusters containing three and four lesions in mouse fibroblasts using a luciferase reporter plasmid. The addition of a third furan did reduce but not eliminate cleavage, while a tandem 8-oxo-7,8-dihydroguanine (8oxoG) immediately 5′ to one furan in a two or three furan cluster decreased DSB formation by a small amount. In vitro studies using nuclear extracts demonstrated that the tandem 8oxoG was not removed under conditions where the furan was cleaved, but the presence of the 8oxoG reduced cleavage at the furan. Interestingly, a cluster of an 8oxoG opposite a furan did not form a DSB in cells. We have shown that Apex1 can cleave these complex clustered lesions in cells. This therefore indicates that Apex1 can generate complex DSBs from clustered lesions consisting of base damage and AP sites. Repair of these complex DSBs may be compromised by the nearby oxidative damage resulting in potentially lethal and biologically relevant damage.     

Radiation chemical mechanisms of single- and double-strand break formation in irradiated SV40 DNA

Using an electrophoresis assay system developed in our laboratory, we have simultaneously measured single- and double-strand DNA breaks (SSBs and DSBs) induced by gamma radiation in small SV40 viral DNA molecules, under conditions of greatly varying radical scavenger concentration and DNA configuration. In our experiments with aqueous solutions of SV40 DNA, we observe that SSB induction is linear with dose (one-hit response), over the entire hydroxyl scavenger efficiency range examined, from approximately 0 to 5 x 10(9) s-1, while DSB induction shifts from having a major quadratic component (two-hit response) at very low scavenger efficiencies to nearly pure linear for efficiencies greater than 10(7) s-1. The mean ratio of SSBs to one-hit DSBs remains relatively constant with increasing scavenger efficiency, decreasing from about 100:1 to 40:1 as the scavenger efficiency increases from 2 x 10(5) s-1 to 5 x 10(9) s-1, and the absolute induction efficiencies for breaks decrease by three orders of magnitude. This decrease takes place primarily at scavenger efficiencies above 1 x 10(8) s-1. Irradiation of intranuclear SV40 minichromosomes induces SSBs and DSBs at nearly the same efficiencies as does irradiation of free DNA at the highest scavenger concentrations examined, and at only about twice the efficiencies observed at -75 degrees C, where direct effects are believed to predominate. Our observations that the linear-quadratic mix of the dose-response curve for DSBs depends critically on scavenger efficiency may help to clarify the considerable confusion in the literature on the shape of such curves. Our observations of a relatively constant ratio between one-hit SSBs and DSBs at low and moderate scavenger efficiencies are in agreement with the recent hypothesis of Siddiqi and Bothe (Radiat. Res. 112, 449-463 (1987)) that, contrary to widely and long-held beliefs, the formation by indirect effects of a one-hit DSB in DNA occurs under these conditions predominantly by a mechanism involving a single OH radical, with a presumed radical transfer between complementary DNA strands. In contrast, our results for strongly protective conditions are not consistent with this hypothesis, but are consistent with the predictions of Ward's hypothesis (Radiat. Res. 86, 185-195, (1981)) that one-hit DSBs from indirect effects are produced predominantly by local clusters of OH radicals from single energy deposition events (locally multiply damaged sites) rather than by single OH radicals.(ABSTRACT TRUNCATED AT 400 WORDS)     

A non-radioactive, PFGE-based assay for low levels of DNA double-strand breaks in mammalian cells

A PFGE method was adapted to measure DNA double-strand breaks (DSBs) in mammalian cells after low (0-25 Gy) doses of ionising radiation. Instead of radionuclide incorporation, DNA staining in the gel by SYBR-Gold was used, which lowered the background of DNA damage and could be applied to non-cycling cells. DSB level was defined as a product of a fraction of DNA released to the gel (FR) and a number of DNA fragments in the gel (DNA(fragm)) and expressed as a percentage above control value. The slope of the dose-response curve was two-fold higher compared to that with FR alone as DSB level indicator (31.4 versus 15.6% per Gy). Two alternative ways were proposed to determine the total amount of DNA, used for FR calculation: measurement of DNA content in a plug not subjected to electrophoresis, with the use of Pico-Green, or estimation of DNA released to the gel from a plug irradiated with 600 Gy of gamma-rays. The limit of DSB detection was 0.25 Gy for human G1-lymphocytes and 0.5-1 Gy for asynchronous cultures of human glioma M059 K and J or mouse lymphoma L5178Y-R and -S cells. Specificity of our PFGE assay to DSB was confirmed by the fact that no damage was detected after treatment of the cells with H(2)O(2), an inducer of single-strand DNA breaks (SSBs). On the contrary, the H(2)O(2) inflicted damage was detected by neutral comet assay, attaining 160% above control (equivalent to 2.5 Gy of X-radiation). DSB rejoining, measured in cells after X-irradiation with a dose of 10 Gy, generally proceeded faster than that measured previously after higher (30-50 Gy) doses of ionising radiation. Clearly seen were defects in DSB rejoining in radiosensitive M059 J and L5178Y-S cells compared to their radioresistant counterparts, M059 K and L5178Y-R. In some cell lines, a secondary post-irradiation increase in DSB levels was observed. The possibility is considered that these additional DSBs may accumulate during processing of non-DSB clustered DNA damage or/and represent early apoptotic events.     

Calculation of radiation-induced DNA damage from photons and tritium beta-particles

Yields of DNA single- and double-strand breaks (SSB and DSB) in nucleosomal DNA were calculated for 137Cs, 70 keV photons and tritium beta-particles by Monte Carlo means. Monte Carlo-generated electron tracks for liquid water were used to model energy deposition. Chemical evolution of a track and interactions between species and DNA following water radiolysis were modelled in an encounter-controlled manner. The calculated relative biological effectiveness (RBE) for DSB production for tritium against 137Cs was 1.2 for the total DSB yield. Tritium beta-particles were slightly more efficient compared to 137Cs in producing complex DSB, defined as DSB accompanied by additional strand breaks. The RBE for complex DSB formation was 1.3. Most complex DSB exhibited associated base damage; the extent of the base damage was similar for all the radiation types considered. Correlated DSB conforming to nucleosome periodicity were observed. However, their frequency was low, of the order of 2% of total DSB. For all the DNA damage endpoints considered and their response to variation of the scavenging environment or DNA conformation no difference was observed between 70 keV photons and tritium beta-particles.     

Nanoscale analysis of clustered DNA damage after high-LET irradiation by quantitative electron microscopy – The heavy burden to repair

Low- and high-linear energy transfer (LET) ionising radiation are effective cancer therapies, but produce structurally different forms of DNA damage. Isolated DNA damage is repaired efficiently; however, clustered lesions may be more difficult to repair, and are considered as significant biological endpoints. We investigated the formation and repair of DNA double-strand breaks (DSBs) and clustered lesions in human fibroblasts after exposure to sparsely (low-LET; delivered by photons) and densely (high-LET; delivered by carbon ions) ionising radiation. DNA repair factors (pKu70, 53BP1, γH2AX, and pXRCC1) were detected using immunogold-labelling and electron microscopy, and spatiotemporal DNA damage patterns were analysed within the nuclear ultrastructure at the nanoscale level. By labelling activated Ku-heterodimers (pKu70) the number of DSBs was determined in electron-lucent euchromatin and electron-dense heterochromatin. Directly after low-LET exposure (5 min post-irradiation), single pKu70 dimers, which reflect isolated DSBs, were randomly distributed throughout the entire nucleus with a linear dose correlation up to 30 Gy. Most euchromatic DSBs were sensed and repaired within 40 min, whereas heterochromatic DSBs were processed with slower kinetics. Essentially all DNA lesions induced by low-LET irradiation were efficiently rejoined within 24 h post-irradiation. High-LET irradiation caused localised energy deposition within the particle tracks, and generated highly clustered DNA lesions with multiple DSBs in close proximity. The dimensions of these clustered lesions along the particle trajectories depended on the chromatin packing density, with huge DSB clusters predominantly localised in condensed heterochromatin. High-LET irradiation-induced clearly higher DSB yields than low-LET irradiation, with up to ∼500 DSBs per μm³ track volume, and large fractions of these heterochromatic DSBs remained unrepaired. Hence, the spacing and quantity of DSBs in clustered lesions influence DNA repair efficiency, and may determine the radiobiological outcome.