Effects of single and split doses of cobalt-60 gamma rays and 14 MeV neutrons on mouse stem cell spermatogonia

The long-term effects of ionizing radiation on male gonads may be the result of damage to spermatogonial stem cells. Doses of 10 cGy to 15 Gy (60)Co gamma rays or 10 cGy to 7 Gy 14 MeV neutrons were given to NMRI mice as single or split doses separated by a 24-h interval. The ratios of haploid spermatids/2c cells and the coefficients of variation of DNA histogram peaks as measures of both the cytocidal and the clastogenic actions of radiation were analyzed by DNA flow cytometry after DAPI staining. The coefficient of variation is not only a statistical examination of the data but is also used here as a measure of residual damage to DNA (i.e. a biological dosimeter). Testicular histology was examined in parallel. At 70 days after irradiation, the relative biological effectiveness for neutrons at 50% survival of spermatogonial stem cells was 3.6 for single doses and 2.8 for split doses. The average coefficient of variation of unirradiated controls of elongated spermatids was doubled when stem cells were irradiated with single doses of approximately 14 Gy (60)Co gamma rays or 3 Gy neutrons and observed 70 days later. Split doses of (60)Co gamma rays were more effective than single doses, doubling DNA dispersion at 7 Gy. No fractionation effect was found with neutrons with coefficients of variation.     

A comparison of gamma and neutron irradiation on Raji cells: effects on DNA damage, repair, cell cycle distribution and lethality.

The Comet assay (microgel electrophoresis) was used to study DNA damage in Raji cells, a B-lymphoblastoid cell line, after treatment with different doses of neutrons (0.5 to 16 Gy) or gamma rays (1.4 to 44.8 Gy). A better growth recovery was observed in cells after gamma-ray treatments compared with neutron treatments. The relative biological effectiveness (RBE) of neutron in cell killing was determined to be 2.5. Initially, the number of damaged cells per unit dose was approximately the same after neutron and gamma-ray irradiation. One hour after treatment, however, the number of normal cells per unit dose was much lower for neutrons than for gamma rays, suggesting a more efficient initial repair for gamma rays. Twenty-four hours after treatment, the numbers of damaged cells per unit dose of neutrons or gamma rays were again at comparable level. Cell cycle kinetic studies showed a strong G2/M arrest at equivalent unit dose (neutrons up to 8 Gy; gamma rays up to 5.6 Gy), suggesting a period in cell cycle for DNA repair. However, only cells treated with low doses (up to 2 Gy) seemed to be capable of returning into normal cell cycle within 4 days. For the highest dose of neutrons, decline in the number of normal cells seen at already 3 days after treatment was deeper compared with equivalent unit doses of gamma rays. Our present results support different mechanisms of action by these two irradiations and suggest the generation of locally multiply damaged sites (LMDS) for high linear energy transfer (LET) radiation which are known to be repaired at lower efficiency.     

Induction and rejoining of DNA double-strand breaks in human cervix carcinoma cell lines of differing radiosensitivity

Five recently established cell lines of human carcinoma of the cervix of varying radiosensitivity have been used to determine whether the induction or rejoining of DNA double-strand breaks (dsb) shows any correlation with radiosensitivity or radiation recovery capacity. Double-strand DNA breaks have been measured using neutral filter elution at pH 9.6. The number of breaks induced immediately after irradiation with doses of 10 to 40 Gy 60Co gamma rays appeared to show some correlation with radiosensitivity particularly after 10 Gy; the two more radiosensitive lines incurred more breaks than the more radioresistant lines. In addition, the shape of the induction curve with dose was linear for the two sensitive lines but curvilinear for the resistant lines. Despite the dose scales being different, this mirrored their respective cell survival curve shapes. After 30 or 50 Gy irradiation, rejoining of breaks appeared to be rapid and almost complete within 60 min at 37 degrees C for the three resistant lines. However, for the sensitive lines, one line (HX160c) in particular exhibited a reduced rate of dsb rejoining. In addition, a residual level of dsb was present in this line even after allowing rejoining for 3 h. While induction and rejoining of DNA dsb therefore appears to be a factor in determining radiosensitivity, at doses relevant to cellular survival (up to 10 Gy), the greater induction of DNA dsb in radiosensitive lines may play a significant role in determining the cellular response to ionizing radiation.     

The response of ataxia-telangiectasia lymphoblastoid cells to neutron irradiation

The response of control and ataxia-telangiectasia (A-T) cells to increasing doses of high-linear-energy-transfer (LET) ionizing radiation (neutrons) was compared. Ataxia-telangiectasia cells were markedly more sensitive to neutron irradiation than were control cells. The D0 value for the two A-T cell lines was 0.4 Gy while the value for controls was approximately 1.4 Gy. Fast neutrons were considerably more effective than gamma rays in inducing cell death in both cell types, but the sensitivity factor remained approximately the same as with gamma rays. A minimal depression of DNA synthesis was observed in ataxia-telangiectasia cells after neutron irradiation, similar to that reported previously after gamma irradiation. The extent of inhibition was not significantly greater in control cells, contrary to that seen with gamma rays. In time-course experiments a significant difference in degree of inhibition of DNA synthesis was observed between the cell types. Low doses of fast neutrons induced a G2-phase delay in both cell types, but the degree and extent of this delay was greater in ataxia-telangiectasia cells as observed previously with low-LET radiation.     

Quantitative measurement of DNA strand breaks and repair in gamma-irradiated human leukocytes from normal and ataxia telangiectasia donors

Fluorimetric analysis of DNA unwinding, which allows measurement of DNA strand breaks in human leukocytes, has been optimized by reducing the amount of cells required for the test and by modifying the DNA alkali unwinding conditions. This permitted measurement of DNA strand-break induction in cells irradiated with low (0.5-7 Gy) or high doses (5-20 Gy) of gamma rays. Linear dose-response curves were obtained for both dose ranges. Presence of cysteamine during irradiation caused a decrease in the extent of DNA strand breaks. The kinetics of the DNA strand-break rejoining process appeared to be biphasic over the dose range of 2-20 Gy when plotted on a linear vs linear axis (percentage of damage as a function of time). Since the rate of disappearance of damaged DNA was similar for any given dose and for all postirradiation incubation times tested, we have expressed the extent of repair after a given postirradiation incubation as the ratio of the slopes of the regression lines obtained from incubated and nonincubated cells. Leukocytes from 25 healthy donors were analyzed to determine an average value for controls. No difference in the level of DNA strand breaks and the rate of repair of these breaks was observed between leukocytes from three ataxia telangiectasia patients and those from normal donors.     

Measurements of alkali-labile DNA damage and protein-DNA crosslinks after 2450 MHz microwave and low-dose gamma irradiation in vitro

In vitro experiments were performed to determine whether 2450 MHz microwave radiation induces alkali-labile DNA damage and/or DNA-protein or DNA-DNA crosslinks in C3H 10T(1/2) cells. After a 2-h exposure to either 2450 MHz continuous-wave (CW) microwaves at an SAR of 1.9 W/kg or 1 mM cisplatinum (CDDP, a positive control for DNA crosslinks), C3H 10T(1/2) cells were irradiated with 4 Gy of gamma rays ((137)Cs). Immediately after gamma irradiation, the single-cell gel electrophoresis assay was performed to detect DNA damage. For each exposure condition, one set of samples was treated with proteinase K (1 mg/ml) to remove any possible DNA-protein crosslinks. To measure DNA-protein crosslinks independent of DNA-DNA crosslinks, we quantified the proteins that were recovered with DNA after microwave exposure, using CDDP and gamma irradiation, positive controls for DNA-protein crosslinks. Ionizing radiation (4 Gy) induced significant DNA damage. However, no DNA damage could be detected after exposure to 2450 MHz CW microwaves alone. The crosslinking agent CDDP significantly reduced both the comet length and the normalized comet moment in C3H 10T(1/2) cells irradiated with 4 Gy gamma rays. In contrast, 2450 MHz microwaves did not impede the DNA migration induced by gamma rays. When control cells were treated with proteinase K, both parameters increased in the absence of any DNA damage. However, no additional effect of proteinase K was seen in samples exposed to 2450 MHz microwaves or in samples treated with the combination of microwaves and radiation. On the other hand, proteinase K treatment was ineffective in restoring any migration of the DNA in cells pretreated with CDDP and irradiated with gamma rays. When DNA-protein crosslinks were specifically measured, we found no evidence for the induction of DNA-protein crosslinks or changes in amount of the protein associated with DNA by 2450 MHz CW microwave exposure. Thus 2-h exposures to 1.9 W/ kg of 2450 MHz CW microwaves did not induce measurable alkali-labile DNA damage or DNA-DNA or DNA-protein crosslinks.     

Protection by WR-3689 against gamma-ray-induced intestinal damage: comparative effect on clonogenic cell survival, mouse survival, and DNA damage

The aminophosphorothioate WR-3689 was characterized for its ability to protect mouse jejunal cells in vivo from single doses of X or gamma radiation. First, the effect of the drug on the survival of jejunal stem cells was examined using a clonogenic end point, the crypt microcolony assay. When WR-3689 was administered 30 min prior to whole-body irradiation, the number of surviving crypt cells was markedly increased at all doses of the drug, although protection began to level out at doses larger than 600 mg/kg. Protection was maximal when the drug was given 30 min before whole-body irradiation and declined rapidly with both shorter and longer intervals. Protection factors (PFs) were obtained by measuring survival curves for clonogenic crypt cells as a function of radiation dose; WR-3689 given 30 min before whole-body irradiation protected jejunum in the microcolony assay with a PF of 1.26 +/- 0.02, 1.50 +/- 0.10, and 1.65 +/- 0.10 at doses of 200, 400, and 800 mg/kg, respectively. Next, the effect of WR-3689 on the survival of jejunal stem cells was determined by assaying the survival of mice given X-ray doses to the whole abdomen in the range leading to death from the gastrointestinal syndrome. The PFs based on the LD50 values for 11-day survival were 1.31 +/- 0.05 (200 mg/kg) and 1.48 +/- 0.05 (400 mg/kg). Crypt-cell survival and animal survival were thus modified to a similar extent by this agent. Finally, the effect of WR-3689 on the induction of DNA single-strand breaks (SSBs) in jejunal cells was measured using an adaptation of the alkaline elution methodology. In mice treated with WR-3689 (400 or 800 mg/kg) 30 min prior to whole-body irradiation with 10 Gy there was no significant reduction in the number of DNA SSBs induced either in samples of the jejunum or in the cycling crypt cells, providing further evidence that there is no simple relationship between the modification of DNA SSBs and the survival of jejunal stem cells.     

Measurement of the initial levels of DNA damage in human lymphocytes induced by 29 kV X rays (mammography X rays) relative to 220 kV X rays and gamma rays

Experiments using the alkaline comet assay, which measures all single-strand breaks regardless of their origin, were performed to evaluate the biological effectiveness of photons with different energies in causing these breaks. The aim was to measure human lymphocytes directly for DNA damage and subsequent repair kinetics induced by mammography 29 kV X rays relative to 220 kV X rays, 137Cs gamma rays and 60Co gamma rays. The level of DNA damage, predominantly due to single-strand breaks, was computed as the Olive tail moment or percentage DNA in the tail for different air kerma doses (0.5, 0.75, 1, 1.5, 2 and 3 Gy). Fifty cells were analyzed per slide with a semiautomatic imaging system. Data from five independent experiments were transformed to natural logarithms and fitted using a multiple linear regression analysis. Irradiations with the different photon energies were performed simultaneously for each experiment to minimize interexperimental variation. Blood from only one male and one female was used. The interexperimental variation and the influence of donor gender were negligible. In addition, repair kinetics and residual DNA damage after exposure to a dose of 3 Gy were evaluated in three independent experiments for different repair times (10, 20, 30 and 60 min). Data for the fraction of remaining damage were fitted to the simple function F(d) = A/(t + A), where F(d) is the fraction of remaining damage, t is the time allowed for repair, and A (the only fit parameter) is the repair half-time. It was found that the comet assay data did not indicate any difference in the initial radiation damage produced by 29 kV X rays relative to the reference radiation types, 220 kV X rays and the gamma rays of 137Cs and 60Co, either for the total dose range or in the low-dose range. These results are, with some restrictions, consistent with physical examinations and predictions concerning, for example, the assessment of the possible difference in effectiveness in causing strand breaks between mammography X rays and conventional (150-250 kV) X rays, indicating that differences in biological effects must arise through downstream processing of the damage.     

DNA damage and biological expression of adenovirus: a comparison of liquid versus frozen conditions of exposure to gamma rays

Human adenovirus type 2 (Ad 2) was irradiated with 137Cs gamma rays in the liquid state at 0 degree C. DNA breaks were correlated with the inactivation of several viral functions and compared to results obtained previously for irradiation of Ad 2 under frozen conditions at -75 degrees C. Irradiation at 0 degree C induced 170 +/- 20 single-strand breaks and 2.6 +/- 0.4 double-strand breaks/Gy/10(12) Da in the viral DNA. Viral adsorption to human KB cells was inactivated with a D0 of 9.72 +/- 1.18 kGy, whereas the inactivation of Ad 2 plaque formation had a D0 of 0.99 +/- 0.14 or 1.1 +/- 0.29 kGy when corrected for the effect of radiation on virus adsorption. For the adsorbed virus, an average of 4.3 +/- 1.7 single-strand and 0.065 +/- 0.02 double-strand breaks were induced in the viral DNA per lethal hit. In contrast, irradiation of Ad 2 at -75 degrees C results in 2.6- to 3.4-fold less DNA breakage per Gy and a 5.6-fold increase in D0 for plaque formation of the adsorbed virus. Furthermore, although host cell reactivation (HCR) of Ad 2 viral structural antigen production for irradiated virus was substantially reduced in the xeroderma pigmentosum fibroblast strain (XP25RO) compared to normal strains for irradiation at -75 degrees C (57% HCR), it was only slightly reduced compared to normal for irradiation at 0 degree C (88% HCR). These results indicate that the spectrum of DNA damage is both quantitatively and qualitatively different for the two conditions of irradiation.     

Induction and rejoining of large DNA fragments after ion irradiation.

Radiation-induced DNA double-strand breaks (DSBs) were analyzed by separating large DNA fragments by pulsed-field gel electrophoresis. Human U-343MG glioma and K562 erythroleukemia cells were irradiated with 60Co gamma rays or nitrogen ions with high linear energy transfer (125 keV/microm). By comparing the fraction of DNA released into the gel below different size thresholds, corresponding to megabase-pair-sized DNA fragments, the relative effectiveness of the nitrogen ions was found to be dependent on both dose and the threshold size used in the evaluation. This dose dependence was most evident for the smallest threshold (6 Mbp) and was due to a linear dose response for release of the fragments for the ions compared to the curvilinear response for the gamma rays. The two curves intersected, and the relative yield of fragments (nitrogen ions/gamma rays) decreased from more than 3 below 1.5 Gy to 0.8 at 30 Gy. For the larger sizes (6-10.5 Mbp), the relative yield was constant at around 0.7. Thus the ion-induced fragments were shifted to smaller sizes compared to the 60Co gamma rays, and the data for nitrogen ions could not be fitted to random fragment distributions at doses < or =20 Gy. From these results, we conclude that a substantial fraction of the DSBs induced by heavy ions were nonrandomly distributed, correlated with DSBs within a region of < or =2 Mbp. After a dose of 20 Gy, the rejoining curves for ion-induced DSBs were different for each fragment size, resulting in different levels of unrejoined breaks after 6 h.     

Chromatin decondensed by acetylation shows an elevated radiation response

V-79 Chinese hamster lung fibroblasts exposed to 5 mM n-sodium butyrate were irradiated with 60Co gamma rays and cell survival was determined by the cell colony assay. In a separate set of experiments the acetylated chromatin obtained from these cells was irradiated and the change of molecular weight of the DNA was evaluated by alkaline sucrose density centrifugation. At a survival level of 10(-2) to 10(-4) cells exposed to butyrate were found to be 1.3-1.4 times more radiosensitive than control cells. Exposure of isolated chromatin to 100 Gy of 60Co gamma irradiation generated 0.9 +/- 0.03 single-strand breaks (ssb) per 10 Gy per 10(8) Da and 2.0 +/- 0.3 ssb/10 Gy/10(8) Da for control and acetylated chromatin, respectively. The elevated radiation sensitivity of chromatin relaxed by acetylation is in good agreement with previous results on chromatin expanded by histone H1 depletion [Heussen et al., Radiat. Res. 110, 84-94 (1987)]. Packing and accessibility of DNA in chromatin appear to be major factors which influence the radiation sensitivity. The intrinsic radiation sensitivity of chromatin in various packing states is discussed in light of the variation of radiation sensitivity of whole cells in the cell cycle which incorporates repair.     

Changes in chromatin conformation during radiation-induced apoptosis in human lymphocytes

Human peripheral lymphocytes in G(0) phase were irradiated with 1-5 Gy of gamma rays. The biochemical and morphological changes characteristic of apoptosis were examined for 72 h after irradiation. In parallel, changes in chromatin conformation were studied by the method of anomalous viscosity time dependence (AVTD) and by measurements of nuclear halo size. An immediate and dose-dependent relaxation of chromatin, which became saturated at doses above 2-3 Gy, was revealed by the AVTD method. The state of relaxed chromatin lasted up to 12-24 h after irradiation, a response considerably longer than the time attributable to repair of radiation-induced DNA breaks. Measurements of nuclear halo size also indicated the initial relaxation of chromatin in the irradiated cells and its subsequent condensation. This condensation of chromatin as revealed with AVTD correlated well with nuclear condensation, as measured with dual fluorescence staining, and with DNA fragmentation, as measured by conventional and pulsed-field gel electrophoresis (PFGE). Late apoptotic cells did not contribute significantly to the AVTD signal, showing that the chromatin of these cells was completely condensed and fragmented.     

A re-examination of the effects of ionizing radiation on lifespan and transformation of human diploid fibroblasts.

Human diploid fibroblasts, strain MRC-5, were sequentially irradiated with 60Co gamma rays at intervals during their in vitro lifespan. The results indicate that 3 or 6 doses of 1 Gy can increase lifespan, and the same was true for cells treated with 3 doses of 3 Gy. Higher doses (5 x 3 Gy) did reduce growth potential, suggesting either that mid-late passage cells become more sensitive to radiation, or that doses beyond a given threshold reduce population lifespan by multiple cellular hits. The life extension induced by gamma rays might be due to an induced hypermethylation of DNA. Alternatively, oxygen radicals produced by irradiation might trigger an adaptive stress response which would remove damaged macromolecules and thereby increase the cells' growth potential. Whichever explanation is correct, the results show that the human fibroblast system is not appropriate for the study of the well known effect of ionizing radiation in shortening the lifespan of experimental animals. Contrary to earlier published results, populations of cells treated with cumulative doses of 15 Gy or 18 Gy and held for nearly 3 months after they had reached senescence (Phase III), produced no foci of transformed cells.     

Physiological and molecular studies on the effect of gamma radiation in fenugreek (Trigonella foenum-graecum L.) plants

This experiment assessed the biochemical changes in fenugreek plants exposed to gamma radiation. Two pot experiments were carried out during two growing seasons of 2015 and 2016. Seeds were subjected to five doses of gamma irradiation (25, 50, 100, 200 and 400?Gy) and were immediately planted into soil pots in a greenhouse. The experimental analysis was performed in M₁ and M₂ generations. Significant differences between irradiated and control plants were detected for most studied characters in M₁ and M₂ generations. It was demonstrated that low doses of gamma irradiation led to gradually increases in growth, yield characters, leaf soluble protein concomitantly with increases in the contents of phenolic and flavonoids compounds particularly at 100?Gy. These changes were accompanied by a substantial increase in ascorbic acid, α-tocopherol and retinol contents. Proline content was increased under all doses of gamma rays in M₁ generation and the highest amount of proline was obtained at 200?Gy with visible decrease in M₂ generation under the same dose. Meanwhile, the highest dose of gamma radiation (400?Gy) decreased all the studied parameters in both mutagenic generations as compared with control plants. In addition, gamma irradiation doses induced changes in DNA profile on using five primers and caused the appearance and disappearance of DNA polymorphic bands with variation in their intensity. These findings confirm the effectiveness of relatively low doses of gamma rays on improving the physiological and biochemical criteria of fenugreek plants.     

DNA double-strand break misrejoining after exposure of primary human fibroblasts to CK characteristic X rays, 29 kVp X rays and 60Co gamma rays

The efficiency of ionizing photon radiation for inducing mutations, chromosome aberrations, neoplastic cell transformation, and cell killing depends on the photon energy. We investigated the induction and rejoining of DNA double-strand breaks (DSBs) as possible contributors for the varying efficiencies of different photon energies. A specialized pulsed-field gel electrophoresis assay based on Southern hybridization of single Mbp genomic restriction fragments was employed to assess DSB induction and rejoining by quantifying the restriction fragment band. Unrejoined and misrejoined DSBs were determined in dose fractionation protocols using doses per fraction of 2.2 and 4.4 Gy for CK characteristic X rays, 4 and 8 Gy for 29 kVp X rays, and 5, 10 and 20 Gy for 60Co gamma rays. DSB induction by CK characteristic X rays was about twofold higher than for 60Co gamma rays, whereas 29 kVp X rays showed only marginally elevated levels of induced DSBs compared with 60Co gamma rays (a factor of 1.15). Compared with these modest variations in DSB induction, the variations in the levels of unrejoined and misrejoined DSBs were more significant. Our results suggest that differences in the fidelity of DSB rejoining together with the different efficiencies for induction of DSBs can explain the varying biological effectiveness of different photon energies.     

The relative biological effectiveness of low doses of 14 MeV neutrons in steady-state murine spermatogenesis as determined by flow cytometry

The relative biological effectiveness of 14 MeV neutrons in the low-dose range < or =1 Gy has been determined in differentiating and differentiated spermatogonia. Male NMRI mice were exposed to single doses of 2 cGy to 3 Gy of (60)Co gamma rays or neutrons. The ratios of testicular S-phase cells, 4c primary spermatocytes, and elongated spermatids were quantified by DNA flow cytometry 2 to 70 days after irradiation and were found to decrease. Histological samples and testis weight were analyzed in parallel. Doses of 2-5 cGy neutrons and 10-50 cGy gamma rays significantly (P<0.05) decreased the proportions of S-phase cells, spermatocytes and elongated spermatids at 4, 14 and 28 days postirradiation. For S-phase cells, the biphasic shape of the cell survival curves was described with a D(50) of 5 cGy neutrons. The D(50) for (60)Co gamma rays and the relative biological effectiveness could not be determined. The relative biological effectiveness of neutrons at 50% reductions of testis weight, primary spermatocytes, and elongated spermatids were 2.5, 10.0 and 6.1, respectively. This in vivo assay is interesting because of its sensitivity at dose ranges that are relevant for exposures in the environment, the workplace and radiotherapy.     

Repair of DNA damage induced by accelerated heavy ions in mammalian cells proficient and deficient in the non-homologous end-joining pathway

Human and rodent cells proficient and deficient in non-homologous end joining (NHEJ) were irradiated with X rays, 70 keV/microm carbon ions, and 200 keV/microm iron ions, and the biological effects on these cells were compared. For wild-type CHO and normal human fibroblast (HFL III) cells, exposure to iron ions yielded the lowest cell survival, followed by carbon ions and then X rays. NHEJ-deficient xrs6 (a Ku80 mutant of CHO) and 180BR human fibroblast (DNA ligase IV mutant) cells showed similar cell survival for X and carbon-ion irradiation (RBE = approximately 1.0). This phenotype is likely to result from a defective NHEJ protein because xrs6-hamKu80 cells (xrs6 cells corrected with the wild-type KU80 gene) exhibited the wild-type response. At doses higher than 1 Gy, NHEJ-defective cells showed a lower level of survival with iron ions than with carbon ions or X rays, possibly due to inactivation of a radioresistant subpopulation. The G(1) premature chromosome condensation (PCC) assay with HFL III cells revealed LET-dependent impairment of repair of chromosome breaks. Additionally, iron-ion radiation induced non-repairable chromosome breaks not observed with carbon ions or X rays. PCC studies with 180BR cells indicated that the repair kinetics after exposure to carbon and iron ions behaved similarly for the first 6 h, but after 24 h the curve for carbon ions approached that for X rays, while the curve for iron ions remained high. These chromosome data reflect the existence of a slow NHEJ repair phase and severe biological damage induced by iron ions. The auto-phosphorylation of DNA-dependent protein kinase catalytic subunits (DNA-PKcs), an essential NHEJ step, was delayed significantly by high-LET carbon- and iron-ion radiation compared to X rays. This delay was further emphasized in NHEJ-defective 180BR cells. Our results indicate that high-LET radiation induces complex DNA damage that is not easily repaired or is not repaired by NHEJ even at low radiation doses such as 2 Gy.     

Evidence from nondenaturing filter elution that induction of double-strand breaks in the DNA of Chinese hamster V79 cells by gamma radiation is proportional to the square of dose

We have used nondenaturing filter elution performed at both pH 7.2 and pH 9.6 to measure the induction of double-strand breaks (DSBs) in the DNA of Chinese hamster V79 cells by 60Co gamma-radiation doses between 10 and 120 Gy. The absolute DSB yields as measured by this assay were determined by using our recent calibration of the assay based upon disintegrations of 125I incorporated into the DNA. An analysis of the dose-response relationship for the induction of DSBs by 60Co gamma rays showed that the number of DSBs induced per dalton of DNA was proportional to the square of the applied dose throughout the dose range used. The contribution made by the dose to the first power was small at pH 9.6 and negligible at pH 7.2. These results suggest that DSB induction in cells by gamma rays may be entirely a two-hit event.     

Truly incomplete and complex exchanges in prematurely condensed chromosomes of human fibroblasts exposed in vitro to energetic heavy ions

Confluent human fibroblast cells (AG1522) were irradiated with gamma rays, 490 MeV/nucleon silicon ions, or iron ions at either 200 or 500 MeV/nucleon. The cells were allowed to repair at 37 degrees C for 24 h after exposure, and a chemically induced premature chromosome condensation (PCC) technique was used to condense chromosomes in the G2 phase of the cell cycle. Incomplete and complex exchanges were analyzed in the irradiated samples. To verify that chromosomal breaks were truly unrejoined, chromosome aberrations were analyzed using a combination of whole-chromosome specific probes and probes specific for the telomere region of the chromosome. Results showed that the frequency of unrejoined chromosome breaks was higher after irradiation with the heavy ions of high LET, and consequently the ratio of incomplete to complete exchanges increased steadily with LET up to 440 keV/microm, the highest LET included in the present study. For samples exposed to 200 MeV/nucleon iron ions, chromosome aberrations were analyzed using the multicolor FISH (mFISH) technique, which allows identification of both complex and truly incomplete exchanges. Results of the mFISH study showed that 0.7 and 3 Gy iron ions produced similar ratios of complex to simple exchanges and incomplete to complete exchanges; these ratios were higher than those obtained after exposure to 6 Gy gamma rays. After 0.7 Gy of iron ions, most complex aberrations were found to involve three or four chromosomes, which is a likely indication of the maximum number of chromosome domains traversed by a single iron-ion track.     

Changes in osteoclasts after irradiation with carbon ion particles

We examined the effects of radiation on decreases in osteoclast numbers after regional irradiation of rats with carbon ions and gamma rays. Male Wistar rats were subjected to hind-leg irradiation with carbon ions (290 MeV/u) or gamma rays at doses of 15, 22.5, or 30 Gy. The effects of carbon ions and gamma rays on osteoclasts were studied using histologic and morphometric methods. At doses of 15 Gy and 22.5 Gy, osteoclast numbers increased transiently until day 5 after irradiation and then decreased rapidly in both the carbon ion and gamma ray irradiation groups. The carbon ion group showed reduced osteoclast size compared with the gamma ray group. Carbon ion irradiation had a more marked effect on osteoclast activity, and suppressed maturation to a greater extent than gamma irradiation. These observations suggest that carbon ion irradiation induces differential modulation of osteoclast growth factor expression.