Irradiation damage in chromatin isolated from V-79 Chinese hamster lung fibroblasts

The effect of chromatin structure on the extent of radiation damage induced by low doses of 100 KeV X rays was investigated using a fluorescent assay for DNA unwinding. Chromatin was isolated from V-79 Chinese hamster lung fibroblast nuclei by partial digestion with micrococcal nuclease. Gel electrophoresis of the isolated DNA showed the molecular weight of the chromatin preparation to be 10.6 X 10(6) with a size range of 6.6-21.7 X 10(6) Da while a size of 10.2 +/- 0.9 X 10(6) Da was found by sedimenting the DNA in alkaline sucrose gradients. The repeat length of V-79 chromatin was found to be 194 +/- 3 bp. The typical nucleosomal repeat structure of the isolated chromatin and that of intact nuclei was identical. Irradiation with 50 and 100 Gy of 100 KeV X rays and analysis by alkaline sucrose density centrifugation indicated that V-79 chromatin sustained 0.56 +/- 0.19 and 0.69 +/- 0.09 single-strand breaks per 10 Gy per 10(8) Da of DNA, respectively. Irradiation with doses of 0.5-3.0 Gy of 100 KeV X rays and analysis by the fluorometric assay showed that the radiation sensitivity of V-79 chromatin decreases sharply on compaction with MgCl2. Histone H1 depletion, which inhibits compaction and causes chromatin to expand by increasing the linker from 26 to 48 bp, results in a considerable increase in the radiation sensitivity. It is concluded that radiation damage sustained by DNA is greatly influenced by chromatin structure.     

Dependence of the yield of DNA double-strand breaks in Chinese hamster V79-4 cells on the photon energy of ultrasoft X rays

Induction of DNA DSBs by low-LET radiations reflects clustered damage produced predominantly by low-energy, secondary electron "track ends". Cell inactivation and induction of DSBs and their rejoining, assayed using pulsed-field gel electrophoresis, were determined in Chinese hamster V79-4 cells irradiated as a monolayer with characteristic carbon K-shell (CK) (0.28 keV), aluminum K-shell (AlK) (1.49 keV), and titanium K-shell (TiK) (4.55 keV) ultrasoft X rays under aerobic and anaerobic conditions. Relative to (60)Co gamma rays, the relative biological effectiveness (RBE) for cell inactivation at 10% survival and for induction of DSBs increases as the photon energy of the ultrasoft X rays decreases. The RBE values for cell inactivation and for induction of DSBs by CK ultrasoft X rays are 2.8 +/- 0.3 and 2.7 +/- 0.3, respectively, and by TiK ultrasoft X rays are 1.5 +/- 0.1 and 1.4 +/- 0.1, respectively. Oxygen enhancement ratios (OERs) of approximately 2 for cell inactivation and induction of DSBs by ultrasoft X rays are independent of the photon energy. The time scale for rejoining of DNA DSBs is similar for both ultrasoft X rays and 60Co gamma rays. From the size distribution of small DNA fragments down to 0.48 kbp, we concluded that DSBs are induced randomly by CK and AlK ultrasoft X rays. Therefore, ultrasoft X rays are more efficient per unit dose than gamma radiation at inducing DNA DSBs, the yield of which increases with decreasing photon energy.     

The maximum low-dose RBE of 17.4 and 40 keV monochromatic X rays for the induction of dicentric chromosomes in human peripheral lymphocytes

Schmid et al. recently reported on the maximum low-dose RBE for mammography X rays (29 kV) for the induction of dicentrics in human lymphocytes. To obtain additional information on the RBE for this radiation quality, experiments with monochromatized synchrotron radiation were performed. Monochromatic 17.4 keV X rays were chosen for comparison with the diagnostic mammography X-ray spectrum to evaluate the spectral influence, while monochromatic 40 keV X rays represent a higher-energy reference radiation, within the experiment. The induction of dicentric chromosomes in human lymphocytes from one blood donor irradiated in vitro with 17.4 keV and 40 keV monochromatic X rays resulted in alpha coefficients of (3.44 +/- 0.87) x 10(-2) Gy(-1) and (2.37 +/- 0.93) x 10(-2) Gy(-1), respectively. These biological effects are only about half of the alpha coefficients reported earlier for exposure of blood from the same donor with the broad energy spectra of 29 kV X rays (mean energy of 17.4 keV) and 60 kV X rays (mean energy of 48 keV). A similar behavior is evident in terms of RBEM. Relative to weakly filtered 220 kV X rays, the RBEM for 17.4 and 40 keV monochromatic X rays is 0.86 +/- 0.23 and 0.59 +/- 0.24, respectively, which is in contrast to the RBEM of 1.64 +/- 0.27 for 29 kV X rays and 1.10 +/- 0.19 for 60 kV X rays. It is evident that the monochromatic radiations are less effective in inducing dicentric chromosomes than broad-spectrum X rays with the corresponding mean energy value. Therefore, it can be assumed that, for these X-ray qualities with broad energy spectra, a large fraction of the effects should be attributed predominantly to photons with energies well below the mean energy.     

Changes in DNA capacity for actinomycin-D binding in nuclei of interphase cells

3H-AMD binding to DNA in interphase nuclei was tested on asynchronous and synchronous LS/BL cell populations under physiological conditions and after exposure to gamma rays (60Co). 3H-AMD binding to DNA in an asynchronous cell population appeared to be nearly constant and independent of 3H-AMD concentration. However, in comparing individual cells, a great variability could be observed. In synchronized cells the DNA accessibility for 3H-AMD binding changed in the course of the cell cycle, with a maximum occurring at the late G1-phase (13.95 X 10(-12) mumol/nucleus) and a minimum at the late G2-phase (2.63 X 10(-12) mumol/nucleus). In irradiated cells the DNA capacity for 3H-AMD binding was growing with the increasing dose (5-80 Gy) from 4.9 to 11.2 X 10(-12) mumol 3H-AMD/nucleus.     

Relative biological effectiveness of the alpha-particle emitter (211)At for double-strand break induction in human fibroblasts

The purpose of this study was to quantify and to determine the distribution of DNA double-strand breaks (DSBs) in human cells irradiated in vitro and to evaluate the relative biological effectiveness (RBE) of the alpha-particle emitter (211)At for DSB induction. The influence of the irradiation temperature on the induction of DSBs was also investigated. Human fibroblasts were irradiated as intact cells with alpha particles from (211)At, (60)Co gamma rays and X rays. The numbers and distributions of DSBs were determined by pulsed-field gel electrophoresis with fragment analysis for separation of DNA fragments in sizes 10 kbp-5.7 Mbp. A non-random distribution was found for DSB induction after irradiation with alpha particles from (211)At, while irradiation with low-LET radiation led to more random distributions. The RBEs for DSB induction were 2.1 and 3.1 for (60)Co gamma rays and X rays as the reference radiation, respectively. In the experiments studying temperature effects, nuclear monolayers were irradiated with (211)At alpha particles or (60)Co gamma rays at 2 degrees C or 37 degrees C and intact cells were irradiated with (211)At alpha particles at the same temperatures. The dose-modifying factor (DMF(temp)) for irradiation of nuclear monolayers at 37 degrees C compared with 2 degrees C was 1.7 for (211)At alpha particles and 1.6 for (60)Co gamma rays. No temperature effect was observed for intact cells irradiated with (211)At. In conclusion, irradiation with alpha particles from (211)At induced two to three times more DSB than gamma rays and X rays.     

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.     

Charged-particle mutagenesis. 1. Cytotoxic and mutagenic effects of high-LET charged iron particles on human skin fibroblasts.

Cytotoxic and mutagenic effects of high-LET charged iron (56Fe) particles were measured quantitatively using primary cultures of human skin fibroblasts. Argon and lanthanum particles and gamma rays were used in comparative studies. The span of LETs selected was from 150 keV/microns (330 MeV/u) to 920 keV/microns (600 MeV/u). Mutations were scored at the hypoxanthine guanine phosphoribosyl transferase (HPRT) locus using 6-thio-guanine (6-TG) for selection. Exposure to these high-LET charged particles resulted in exponential survival curves. Mutation induction, however, was fitted by the linear model. The relative biological effectiveness (RBE) for cell killing ranged from 3.7 to 1.3, while that for mutation induction ranged from 5.7 to 0.5. Both the RBE for cell killing and the RBE for mutagenesis decreased with increasing LET over the range of 1.50 to 920 keV/microns. The inactivation cross section (sigma i) and the action cross section for mutation induction (sigma m) ranged from 32.9 to 92.0 microns2 and 1.45 to 5.56 X 10(-3) microns2; the maximum values were obtained by 56Fe with an LET of 200 keV/microns. The mutagenicity (sigma m/sigma i) ranged from 2.05 to 7.99 X 10(-5) with an inverse relationship to LET.     

The complexity of radiation-induced DNA damage as revealed by exposure to cell extracts.

The rejoining of single-strand breaks (SSBs) induced in plasmid DNA in the presence of 10 mmol dm(-3) Tris scavenger by aluminum K (Al(K)) ultrasoft X rays has been compared with that for SSBs induced by gamma radiation. The Al(K) ultrasoft X rays interact to produce low-energy secondary electrons, which are thought to be the main contributors to the formation of complex damage by low-LET radiations. The rejoining of radiation-induced SSBs was investigated using human whole cell extracts. The efficiency of rejoining of SSBs induced by Al(K) ultrasoft X rays is less than that observed for gamma-ray-induced SSBs. From the similarity of the extent of rejoining of SSBs induced by gamma rays under aerobic and anaerobic conditions, the chemical nature of the stand break termini does not significantly influence SSB rejoining. A simple nick induced in plasmid DNA by gpII protein is rejoined rapidly compared with the slower rejoining processes for radiation-induced SSBs. Therefore, ligation is not rate-determining in processing radiation-induced SSBs. This study provides further evidence that nonrejoining of radiation-induced SSBs reflects the complexity of DNA damage. From comparison of the extent of rejoining of SSBs induced by different radiations, it is inferred that double-strand breaks represent only a minor component of the overall yield of complex damage.     

The effectiveness of monoenergetic neutrons at 565 keV in producing dicentric chromosomes in human lymphocytes at low doses

The induction of dicentric chromosomes in human lymphocytes from one individual irradiated in vitro with monoenergetic neutrons at 565 keV was examined to provide additional data for an improved evaluation of neutrons with respect to radiation risk in radioprotection. The resulting linear dose-response relationship obtained (0.813 +/- 0.052 dicentrics per cell per gray) over the dose range of 0.0213-0.167 Gy is consistent with published results obtained for irradiation with neutrons from different sources and with different spectra at energies lower than 1000 keV. Comparing this value to previously published "average" dose-response curves obtained by different laboratories for (60)Co gamma rays and orthovoltage X rays resulted in maximum RBEs (RBE(m)) of about 37 +/- 8 and 16 +/- 4, respectively. However, when our neutron data were matched to low-LET dose responses that were constructed several years earlier for lymphocytes from the same individual, higher values of RBE(m) resulted: 76.0 +/- 29.5 for (60)Co gamma rays and 54.2 +/- 18.4 for (137)Cs gamma rays; differentially filtered 220 kV X rays produced values of RBE(m) between 20.3 +/- 2.0 or 37.0 +/- 7. 1. The results highlight the dependence of RBE(m) on the choice of low-LET reference radiation and raise the possibility that differential individual response to low-LET radiations may need to be examined more fully in this context.     

Repair capacity and kinetics in spheroids from a lung metastasis of a human soft tissue sarcoma: a growth delay study.

Spheroids grown from the human cell line EF8 of a lung metastasis of a human malignant fibrous histiocytoma were given fractionated irradiation with 60Co gamma rays at passages 31 and 32. The mean diameter of the spheroids at the time of treatment was 250 microns. Growth delay was used as the end point in these studies. Two experiments were carried out to determine the capacity and kinetics of repair of sublethal damage. In the first experiment, one, two, and five fractions were given at three or four dose levels with fixed intervals of 360 min. In the second experiment, schedules with two and four dose fractions and intervals of 0, 20, 60, 120, and 360 min were used, each at two dose levels. Data analysis was performed by a direct method based on the alpha/beta model and first-order repair kinetics of radiation damage. In both experiments, the alpha/beta value of EF8 spheroids was estimated to be about 8 (6-10) Gy. The rate constant of repair, mu, and its 95% confidence interval were estimated to be 0.62 (0.40-0.84) 10(-2) min-1, equivalent to a half-time of repair (T1/2) of 112 (83-172) min. A more detailed analysis of the data of the second experiment revealed a significant dependence of the rate constant of repair, mu, on the total radiation effect induced by the fractionated radiation treatments with short overall times. With increasing level of effect, mu decreased. These data indicate that the half-time of recovery of a human tumor can be longer than that of the surrounding normal tissue, in this case lung, at least for a limited range of doses and for some fractionation schedules.     

Conformational properties of DNA after exposure to gamma rays and neutrons

DNA aqueous solutions were irradiated with 0-40 Gy of 60Co gamma rays and 0-1.5 Gy of (Pu-Be) neutrons. Thermal transition spectrophotometry (TTS) was used to trace the changes in the DNA conformation at the above doses. Previous results using the perturbed angular correlation (PAC) method were used to complement to the current analysis. The TTS and PAC methods are two different approaches to the study of the effects of radiation on DNA. Both showed that neutrons are more effective than gamma rays in inducing DNA damage. The TTS method showed that neutrons are 11 +/- 5 times more efficient than gamma rays, while the PAC method had shown this value to be 34 +/- 4. From the current study we deduced that the radiation damage to DNA is not a spontaneous effect but rather is an ensemble of damaging events that occur asynchronously. Any single method selected for the study of such damages can concentrate on only a part of the damage, leading to over- or underestimation of the relative effectiveness of the neutrons.     

Kinetics of murine type C virus-specific DNA synthesis newly infected cells.

Replicating transforming functions of Rauscher leukemia virus (RLV) and the RLV pseudotype of Moloney sarcoma virus in mouse embryo fibroblasts were found to be most sensitive to inhibition by cytosine arabinoside (ara-C) 30 to 90 min after infection. The initiation of intracellular RLV DNA synthesis was detected by nucleic acid hybridization within this time interval. Treatment of infected cells with cytosine arabinoside abolished RLV DNA synthesis. Peak synthesis of the DNA complementary to the infecting RLV genome, the (-) strand, occurred 40 to 60 min after infection. During this interval two s two species of DNA were observed with estimated molecular weights of 0.5 X 10(5) to 1.0 X 10(5) and 3 X 10(6). Peak synthesis of the (+) strand viral DNA occurred 50 to 70 min after infection. The initial species detected had a molecular weight of 1.5 X 10(5) to 4.0 X 10(5) which shifted as a function of time to 3 X 10(6). Both (+) strand species were initially detected in the cytoplasm followed by a rapid (10-min interval) appearance of the faster-sedimenting species in the nucleus. The virus-specific (-) and (+) strand DNA species are presumably unintegrated intermediates in provirus formation.     

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 neoplastic transformation potential of mammography X rays and atomic bomb spectrum radiation

Considerable controversy currently exists regarding the biological effectiveness of 29 kVp X rays which are used for mammography screening. This issue must be resolved to enable proper evaluation of radiation risks from breast screening. Here a definitive assessment of the biological effectiveness of 29 kVp X rays compared to the quality of radiation to which the atomic bomb survivors were exposed is presented for the first time. The standard radiation sources used were (a) an atomic bomb simulation spectrum and (b) 2.2 MeV electrons from a strontium-90/yttrium-90 (90Sr/90Y) radioactive source. The biological end point used was neoplastic transformation in vitro in CGL1 (HeLa x human fibroblast hybrid) cells. No significant difference was observed for the biological effectiveness of the two high-energy sources for neoplastic transformation. A limiting relative biological effectiveness (RBE(M)) of 4.42 +/- 2.02 was observed for neoplastic transformation by 29 kVp X rays compared to these two sources. This compares with values of 4.67 +/- 3.93 calculated from previously published data and 3.58 +/- 1.77 when the reference radiation was 200 and 220 kVp X rays. This suggests that the risks associated with mammography screening may be approximately five times higher than previously assumed and that the risk-benefit relationship of mammography exposures may need to be re-examined.     

Qualitative and quantitative analyses of the decomposition products that arise from the exposure of thymine to monochromatic ultrasoft X rays and 60Co gamma rays in the solid state

HPLC analyses of condensed thymine irradiated with monochromatic synchrotron ultrasoft X rays in the energy region around nitrogen and oxygen K-shell edges were performed. Cobalt-60 gamma rays were used as a reference radiation. The radiation chemical dose response of each separated thymine decomposition product was also determined. Uracil (U), 5-(hydroxymethyl)uracil (HMU), 5,6-dihydrothymine (DHT), 5-formyluracil (foU) and four main unknown products were found in the HPLC chromatogram of the sample irradiated with ultrasoft X rays in vacuo. Similar spectra of the products were also found in the gamma-ray experiment; however, some unknown products that appeared after elution of the thymine peak were significantly larger than those in the ultrasoft X- ray experiment. This result indicates the difference in radiation quality. The G value of DHT produced by gamma radiation was 10 times larger than those produced by the ultrasoft X- ray photons with energies of 395 and 407 eV corresponding to below and on the nitrogen K-shell edge, respectively. This result suggests that the differences in the photon energy and/ or in the energy spectra of the secondary electron between ultrasoft X rays and gamma rays are causing differences in the process of the radiation chemistry. Moreover, the yields of all the thymine decomposition products induced by 538 eV photons (oxygen K-shell edge) were significantly smaller than those induced by photons around the nitrogen K-shell edge. The K-shell excitation of oxygen in thymine may efficiently promote the production of small thymine fragments susceptible to desorption from the sample.     

DNA supercoiling changes in nucleoids from irradiated L5178Y-S and -R cells

DNA supercoiling ability was assayed following irradiation in two cell lines of differing radiosensitivity, L5178Y-S (LY-S) and L5178Y-R (LY-R). Cells treated with NaCl and Triton X-100 were exposed to increasing concentrations of the fluorescent, DNA-intercalating dye, propidium iodide (PI), and the diameter of the resulting fluorescent halo of DNA was measured. As the PI concentration was increased from 0.5 to 5 micrograms/ml, halo diameter increased from 20-25 to 45-55 microns due to the unwinding of the DNA supercoils. This process was similar for both cell lines under all conditions studied. As the PI concentration was increased to 50 micrograms/ml, the halo rewound to a diameter of 25-30 microns in unirradiated cells from both lines. However, following exposure to 3-12 Gy of 137Cs gamma rays, the ability of the DNA to be rewound was inhibited in a dose-dependent manner. Rewinding inhibition was greater in LY-S cells than in LY-R cells. Since the induction of DNA damage (e.g., single-strand DNA breaks) appears to be the same for both cell lines, this result implies that a similar extent of damage results in a greater loss of topological constraints on the DNA loops in LY-S. Such a change might be related to the protein composition of the nucleoid cores. One-dimensional sodium dodecyl sulfate-polyacrylamide gel electrophoresis demonstrated that nucleoids from LY-S cells were missing a 55-kDa protein present in LY-R.     

Microdosimetry for boron neutron capture therapy.

Preclinical studies for boron neutron capture therapy (BNCT) using epithermal neutrons are ongoing at several laboratories. The absorbed dose in tumor cells is a function of the thermal neutron flux at depth, the microscopic boron concentration, and the size of the cell. Dosimetry is therefore complicated by the admixture of thermal, epithermal, and fast neutrons, plus gamma rays, and the array of secondary high-linear-energy-transfer particles produced within the patient from neutron interactions. Microdosimetry can be a viable technique for determining absorbed dose and radiation quality. A 2.5-cm-diameter tissue-equivalent gas proportional counter has been built with 50 parts per million (ppm) 10B incorporated into the walls and counting gas to simulate the boron uptake anticipated in tumors. Measurements of lineal energy (y) spectra for BNCT in simulated volumes of 1-10 microns diameter show a dose enhancement factor of 4.3 for 30 ppm boron, and a "y" of 250 keV/microns for the boron capture process. Chamber design plus details of experimental and calculated linear energy spectra will be presented.     

Changes in DNA flexibility after irradiation with gamma rays and neutrons studied with the perturbed angular correlation method

Neutron and gamma irradiation of buffered solutions of calf thymus DNA resulted in changes in the dynamics of the macromolecule. In the low-dose region (0.8-10 cGy of 239Pu-Be neutrons and 0.34-3 Gy of 60Co gamma rays), the flexibility of DNA decreased as indicated by slower rotation of the molecules. Neutrons appeared to be approximately 35 times more effective than 60Co gamma rays. The rotational correlation time, tau C, was measured using the perturbed angular correlation (PAC) method. Its variation appears to follow a linear-exponential behavior. An attempt is made to formulate this behavior as a function of the energy deposited on the macromolecule (radiation dose), the average threshold energy (dose) required to form new lesions, and the available population of intact DNA sites.     

Induction of sperm head abnormalities by incorporated radionuclides: dependence on subcellular distribution, type of radiation, dose rate, and presence of radioprotectors

In contrast to the biological effects caused by exposure to external beams of radiation, the effects of tissue-incorporated radionuclides are highly dependent on the type of radiation emitted and on their distribution at the macroscopic, microscopic, and subcellular levels, which are in turn determined by the chemical nature of the radionuclides administered. Induction of abnormalities of sperm heads in mice is investigated in this work after the injection of a variety of radiochemicals including alpha emitters. When the initial slopes of the dose-response curves are used to compare the relative biological effectiveness (RBE) of different radiocompounds, the alpha particles emitted in the decay of 210Po are more effective than Auger electrons emitted by 125I incorporated in the DNA of the spermatogonial cells, and both emissions are more effective than X rays. It is also shown that the Auger emitters (125I, 111In) distributed in the cell nucleus are more efficient in producing abnormalities than the same radionuclides localized in the cytoplasm. These findings are consistent with our earlier observations, where spermatogonial cell survival is assayed as a function of the testicular absorbed dose. Further, chronic irradiation of testis with gamma rays from intratesticularly administered 7Be is about three times more effective in causing abnormalities than a single acute exposure to 120-kVp X rays. The resulting RBE values correlate well with our data on sperm head survival with the same radiocompounds. Finally, the radioprotector cysteamine, when administered in small, nontoxic amounts, significantly reduces the incidence of sperm abnormalities from alpha-particle radiation as well as emissions from 125I incorporated into DNA, the dose reduction factors being 10 and 14, respectively.     

Accelerated heavy particles and the lens. VI. RBE studies at low doses

We report on the prevalence, hazard, and relative biological effectiveness (RBE) for various stages of lens opacification in rats induced by very low doses of fast argon ions of LET 88 keV/microns, compared to those for X rays. Doses of argon ions from 0.01 to 0.25 Gy were used and RBEs of these ions relative to X rays estimated using a nonparametric technique. At the end of the follow-up period, which encompasses a significant fraction of the animals' lifetime, 90% confidence intervals for the RBE of the argon ions relative to X rays were 4-8 at 0.25 Gy, 10-40 at 0.05 Gy, and 50-100 at 0.01 Gy. Our results are consistent with the point-estimate neutron RBEs in Japanese A-bomb survivors, though broad confidence bounds are present in the Japanese results. If a reasonable extrapolation to higher doses is used, our results are also consistent with data reported earlier at higher doses for argon-ion cataractogenesis in rats, mice, and rabbits. We conclude from these results that at very low doses the RBE for cataractogenesis from HZE particles in space is considerably more than 20, and use of a quality factor of at least 50 would be prudent.