The question of relative biological effectiveness and quality factor for auger emitters incorporated into proliferating mammalian cells

The problem of determining RBE values for Auger emitters incorporated into proliferating mammalian cells is examined. In general, the reference radiation plays a key role in obtaining experimental RBE values. Using survival of cultured Chinese hamster V79 cells as the experimental model, new data are provided regarding selection of a reference radiation for internal Auger emitters. These data show that gamma rays delivered acutely (137Cs) are more than twice as lethal as gamma rays delivered chronically with an exponentially decreasing dose rate (99mTc). The results confirm that the reference radiation should be delivered chronically in a manner consistent with the extended exposure received by the cells in the case of incorporated radionuclides. Through a direct comparison of the radiotoxicity of Auger emitters and alpha emitters, the high RBE values reported for DNA-bound Auger emitters are confirmed. These studies reveal that the DNA binding compound [125I]iododeoxyuridine (125IdU) is about 1.6 times more effective in killing V79 cells than 5.3 MeV alpha particles from intracellularly localized 210Po-citrate. In addition, toxicity studies with the radiochemicals 125IdU and [125]-iododeoxycytidine (125IdC) establish the equivalence of the radiosensitivity of thymine and cytosine base sites in the DNA. In view of these results, and information already available, the question of establishing quality factors for Auger emitters is considered. Finally, a method for calculation of the dose equivalent for internal Auger emitters is advanced.     

Radiotoxicity of 125I in mammalian cells

The radiotoxicity of 125I in Chinese hamster V79 lung fibroblasts has been studied following extracellular (Na125I), cytoplasmic [125I]iododihydrorhodamine (125I-DR), and nuclear (125IUdR) localization of the radionuclide. Exposure of the cells for 18 h to Na125I (less than or equal to 7.4 MBq/ml) had no effect on survival. A similar exposure to 125I-DR produced a survival curve with a distinct shoulder and with a mean lethal dose (D37) of 4.62 Gy to the nucleus. While this value compares well with the 5.80 Gy X-ray D37 dose, it is in contrast to the survival curve obtained with DNA-bound 125IUdR which is of the high LET type and has a D37 of 0.80 Gy to the nucleus. Furthermore, when the uptake of 125I into DNA is reduced by the addition of nonradioactive IUdR or TdR to the medium and the survival fraction is determined as a function of 125I contained in the DNA, a corresponding increase in survival is observed. This work demonstrates the relative inefficiency of the Auger electron emitter 125I when located in the cytoplasm or outside the cell. It indicates that a high dose deposited within the cytoplasm contributes minimally to radiation-induced cell death and that radiotoxicity depends not upon the specific activity of IUdR but upon the absolute amount of 125I that is associated with nuclear DNA.     

The Auger electron dosimetry of indium-111 in mammalian cells in vitro

Most of the radionuclides used in the formulation of radiopharmaceuticals emit Auger electrons when they undergo radioactive decay. The release of these low-energy electrons at extracellular sites produces little direct damage to intracellular structures. However, many radiopharmaceuticals, or their metabolites, can be transported into the cell where the Auger electrons have the potential to damage nearby intracellular macromolecules, including DNA. In this preliminary study, chromosome damage, expressed as 60Co equivalent doses, and the effects on cell division following treatment with intracellular and extracellular 111In were measured in Chinese hamster V79 cells. The chromosome aberration yield in cells irradiated by intracellular 111In indicated that damage was induced at a rate of 7.2 X 10(-4) Gy/decay for levels of activity up to 0.075 Bq/cell and 4.5 X 10(4) and 2.9 X 10(4) Gy/decay for intermediate (0.204 Bq/cell) and high (0.389 Bq/cell) levels, respectively. Extracellular 111In-chloride produced damage at a rate of about 6.1 X 10(-12) Gy/decay. As little as 4.4 mBq/cell (about 4.4 X 10(3) Bq/ml of culture) of intracellular 111In was able to affect cell division, whereas extracellular 111In at 1.150 MBq/ml of culture had little effect. These data indicate that the Medical Internal Radiation Dose and International Committee on Radiation Units methods for organ dosimetry may underestimate the potential of intracellular Auger electron emitters to produce radiation damage.     

Relative biological effectiveness of accumulated 125IdU and 125I-estrogen decays in estrogen receptor-expressing MCF-7 human breast cancer cells

The therapeutic potential for delivering a cytotoxic dose of radiation (using the decay of Auger-electron emitters) to the cell nucleus of cancer cells that express estrogen receptors (ERs) by radiolabeled estrogen was investigated in the ER-expressing human breast cancer cell line, MCF-7. The radiolabeled estrogen/ER complex irradiates the cell nucleus by binding specific DNA sequences called estrogen response elements (EREs). Cell clonogenicity and induction of DNA double-strand breaks (DSBs) by gamma radiation or accumulation of (125)I-iododeoxyuridine ((125)IdU) or E-17alpha[(125)I]iodovinyl-11betamethoxyestradiol ((125)IVME2) decays were determined. MCF-7 cells were efficiently killed by accumulation of (125)IdU (D(0) = 30 decays per cell) and (125)IVME2 decays (D(0) = 28 decays per cell). DNA DSBs were induced by the accumulation of (125)IdU (approximately 3750 decays per cell required to reduce the mean value of the elution profile to 50%) or (125)IVME2 decays (approximately 465 decays per cell required to reduce the mean value to 50%). For survival of MCF-7 cells after gamma irradiation, the D(0) was 1 Gy, and approximately 65 Gy was required to reduce the mean value to 50% for induction of DSBs. The RBE values for cell killing and induction of DSBs by (125)IVME2 relative to gamma radiation were 4.8 and 18.8, respectively. The RBE values for cell killing and induction of DSBs by (125)IdU relative to gamma radiation were 4.5 and 2.3, respectively. Cell killing in a manner similar to that induced by high-LET radiation and the high RBE for induction of DSBs by (125)IVME2 in the ER-expressing MCF-7 cells provide a biological rationale for the use of Auger electron-emitting radionuclides covalently bound to estrogen to deliver a cytotoxic dose of radiation to ER-positive cancers.     

Relative biological effectiveness of high-energy iron ions for micronucleus formation at low doses

Dose-response curves for micronucleus (MN) formation were measured in Chinese hamster V79 and xrs6 (Ku80(-)) cells and in human mammary epithelial MCF10A cells in the dose range of 0.05-1 Gy. The Chinese hamster cells were exposed to 1 GeV/nucleon iron ions, 600 MeV/nucleon iron ions, and 300 MeV/nucleon iron ions (LETs of 151, 176 and 235 keV/microm, respectively) as well as with 320 kVp X rays as reference. Second-order polynomials were fitted to the induction curves, and the initial slopes (the alpha values) were used to calculate RBE. For the repair-proficient V79 cells, the RBE at these low doses increased with LET. The values obtained were 3.1 +/- 0.8 (LET = 151 keV/microm), 4.3 +/- 0.5 (LET = 176 keV/microm), and 5.7 +/- 0.6 (LET = 235 keV/microm), while the RBE was close to 1 for the repair-deficient xrs6 cells regardless of LET. For the MCF10A cells, the RBE was determined for 1 GeV/nucleon iron ions and was found to be 5.5 +/- 0.9, slightly higher than for V79 cells. To test the effect of shielding, the 1 GeV/nucleon iron-ion beam was intercepted by various thicknesses of high-density polyethylene plastic absorbers, which resulted in energy loss and fragmentation. It was found that the MN yield for V79 cells placed behind the absorbers decreased in proportion to the decrease in dose both before and after the iron-ion Bragg peak, indicating that RBE did not change significantly due to shielding except in the Bragg peak region. At the Bragg peak itself with an entrance dose of 0.5 Gy, where the LET is very high from stopping low-energy iron ions, the effectiveness for MN formation per unit dose was decreased compared to non-Bragg peak areas.     

Cytotoxicity,genotoxicity and intracellular distribution of the Auger electron emitter <Superscript>65</Superscript>Zn in two human cell lines

Cell survival, induction of apoptosis, and micronucleus formation have been examined in non-transformed human amnion fluid fibroblast-like (AFFL) cells and in a human squameous cell carcinoma (SCL-II) cell line after exposure to the Auger electron emitter ⁶⁵Zn and after external low-LET radiation. Cellular uptake and subcellular distribution of ⁶⁵Zn²⁺ were studied in vitro and the absorbed radiation dose was calculated applying analytical dosimetry models. Auger electrons generated during decay of ⁶⁵Zn induced a prominent decrease in cell survival and increased the levels of apoptotic as well as micronucleated cells when compared to external low-LET irradiation. Relative biological effectiveness has been determined for cell survival (RBE ~4), micronucleus formation (RBE ~2) and apoptosis induction (RBE ~5–8) in SCL-II cells and for micronucleus formation (RBE ~4–5) and apoptosis induction (RBE ~6–10) in AFFL cells, respectively. This demonstrates a general enhanced biological effectiveness of ⁶⁵Zn in both investigated cell lines when compared to external low-LET radiation. The distribution pattern of intracellular Zn²⁺ was found to be non-uniform, showing enhanced amounts of Zn²⁺ in the perinuclear region and low amounts inside the cell nucleus, suggesting a major energy deposition close to the nuclear envelope.     

Radiobiology of ultrasoft X rays. II. Cultured C3H mouse cells (10T1/2)

In the first paper of this series (Radiat. Res. 110, 396-412 (1987], using V79 cells, we reported that the relative biological effectiveness (RBE) of ultrasoft X rays was found to increase with decreasing energy, and the oxygen enhancement ratio (OER) was found to decrease with decreasing energy. In this report, we present RBE and OER results for 10T1/2 cells that are known to grow uniformly flat and are considerably thinner than V79 cells. Thus the variation in dose across the cell nucleus is considerably reduced. The OER results agree well with our earlier V79 results. However, the RBE values for 10T1/2 cells compared to V79 cells are systematically less for all soft X rays and especially for 0.28 keV carbon-K (1.3 compared to 3.4 for V79 cells). Some plausible explanations are presented to reconcile the apparent discrepancy between V79 and 10T1/2 results.     

Radiobiology of ultrasoft X rays. IV. Flat and round-shaped hamster cells (CHO-10B, HS-23)

The results reported earlier in this series indicated that the relative biological effectiveness (RBE) of ultrasoft X rays decreases with decreasing cell thickness, approaching unity for the thinnest cells used, plateau-phase human skin fibroblasts (HSF). The possible dependence of RBE on the configuration of the cell nucleus is investigated further in this paper using two CHO cell lines that attach well and have similar intrinsic radiosensitivities to 60Co gamma rays. One of the lines forms monolayers similar to V79 cells, while the other remains more spherical during growth. We find an increasing RBE with decreasing X-ray energy for both of these cell lines, consistent with our results using V79 cells. Also consistent with our results obtained with 10T1/2 and HSF cells, we find an increasing RBE with increasing cell thickness. The possible dependence of RBE on radiosensitivity and the use of the concept of mean dose for ultrasoft X rays is discussed.     

The radiation dose to cells in vitro from intracellular indium-111

Most of the radionuclides used in nuclear medicine emit low energy Auger electrons following radioactive decay. These emissions, if intracellular, could irreparably damage the radiosensitive structures of the cell. The resulting radiation dose, which is a measure of biological damage in the affected cell, could be many times the average radiation dose to the associated organ. In this series of experiments, the radiation dose to the nucleus of a chinese hamster V79 cell was determined for the intracellular radiopharmaceutical 111indium-oxine. Assuming the cell nucleus to be the radiosensitive volume, the radiation dose would be primarily due to the low energy Auger electrons. A much smaller dose would be absorbed from the penetrating X- and gamma-rays and internal conversion electrons released from other radiolabelled cells in the culture. The radiation dose to the cell from the intranuclear decay of 111In was empirically established from cell survival studies to be 3.5 mGy/decay, using cobalt-60 as a reference radiation. The average dose to V79 cells from extracellular 111In (i.e., from 111In located outside the target cell) was calculated to be 5.8 pGy/decay. This suggests that for an intracellular radiopharmaceutical, the radiation dose of consequence would be delivered by the low energy Auger electrons. In contrast, Auger electrons from an extracellular radiopharmaceutical could not directly damage the cell nucleus and therefore would not contribute to the radiation dose.     

Toxicity of DNA-incorporated iodine-125: quantifying the direct and indirect effects

To understand the biophysical mechanism(s) underlying the induction of cell death by the decay of the Auger electron emitter iodine-125 in DNA, Chinese hamster V79 lung fibroblasts were labeled with 5-[(125)I]iodo-2'-deoxyuridine ((125)IdU) for two doubling times and frozen and stored at -135 degrees C in the presence of 0.26-3.0 M dimethyl sulfoxide (DMSO), which acts simultaneously as a cryoprotector and a hydroxyl radical scavenger. After the accumulation of (125)I decays, the cells were defrosted and their survival was determined. Within the range of the number of decays examined (up to 470 disintegrations per cell), the survival curves are exponential. The dependence of the D(37) on DMSO concentration is triphasic and seems to reach a plateau at approximately 1.3 M. By extrapolating to infinite DMSO concentration, we estimate the D(37) for maximal hydroxyl radical scavenging to be 411 +/- 36 disintegrations per cell. To determine the D(37) in the absence of DMSO, we extrapolate the D(37) curve to zero concentration, and a D(37) of 54 +/- 5 disintegrations per cell is obtained. The maximal dose modification factor, calculated as the ratio of the D(37) at infinite DMSO concentration (i.e. direct effects only) to the D(37) at zero DMSO concentration (i.e. direct and indirect effects), is 7.6 +/- 1.0. By inference, approximately 90% of the radiotoxic effects of DNA-incorporated (125)I are due to indirect mechanisms.     

Relative biological effectiveness of high-energy photons (up to 50 MV) and electrons (50 MeV)

In vitro studies of the relative biological effectiveness (RBE) of 50-MV X rays have shown an RBE of 1.1 relative to 4-MV X rays. This will be important in clinical radiotherapy. The aim of this study was to verify these results and to investigate whether photonuclear processes might cause the difference in RBE. To do so, 50- and 20-MV X rays and 50-MeV electrons were investigated with respect to RBE. Chinese hamster V79 cells were irradiated in a specially designed system which allows for a high reproducibility of geometry and dosimetry. Fractionation experiments were also carried out to establish the RBE at the clinically relevant dose level, 2 Gy. Fricke dosimetry was used, and the results were confirmed with ionization chamber measurements. The RBE for 50-MV X rays was estimated to be 1.14 at a surviving fraction of 0.1 and 1.12 at a surviving fraction of 0.01. The RBEs for the other qualities were equal to one. The RBE calculated for the 2 Gy/fraction experiments was 1.17.     

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.     

Clonogenic survival of human keratinocytes and rodent fibroblasts after irradiation with 25 kV x-rays

Low energy x-rays (E_ph 50 keV) are widely used in diagnostic radiology and radiotherapy. However, data on their relative biological effectiveness (RBE) are scarce. Of particular importance for risk estimation are the RBE values of x-rays in the range which is commonly used in mammography (10–30 keV). We have determined clonogenic survival after low-energy x-ray irradiation for three cell lines: primary human epidermal keratinocytes (HEKn), mouse fibroblasts (NIH/3T3) and Chinese hamster fibroblasts (V79). Experiments were performed with a 25 kV x-ray tube and compared to 200 kV x-rays as a reference. Compared to the effect of 200 kV x-rays, irradiation with 25 kV x-rays resulted in a decreased survival rate in the murine fibroblasts, but not in the human epithelial cell line. The RBE value was calculated for 10% surviving fraction. For HEKn cells, RBE was 1.33±0.27, for NIH/3T3 cells 1.25±0.07 and for V79 cells 1.10±0.09, respectively. No consistently increased RBE was observed in the various cell lines. Nevertheless, a potential of increased cytogenetic changes has to be considered for risk estimation of low-energy x-rays.     

Protection by DMSO against cell death caused by intracellularly localized iodine-125, iodine-131 and polonium-210

The mechanisms by which DNA-incorporated radionuclides impart lethal damage to mammalian cells were investigated by examining the capacity of dimethyl sulfoxide (DMSO) to protect against lethal damage to Chinese hamster V79 cells caused by unbound tritium ((3)H(2)O), DNA-incorporated (125)I- and (131)I-iododeoxyuridine ((125)IdU, (131)IdU), and cytoplasmically localized (210)Po citrate. The radionuclides (3)H and (131)I emit low- and medium-energy beta particles, respectively, (125)I is a prolific Auger electron emitter, and (210)Po emits 5.3 MeV alpha particles. Cells were radiolabeled and maintained at 10.5 degrees C for 72 h in the presence of different concentrations of DMSO (5-12.5% v/v), and the surviving fraction compared to that of unlabeled controls was determined. DMSO afforded no protection against the lethal effects of the high-LET alpha particles emitted by (210)Po. Protection against lethal damage caused by unbound (3)H, (131)IdU and (125)IdU depended on the concentration of DMSO in the culture medium. Ten percent DMSO provided maximum protection in all cases. The dose modification factors obtained at 10% DMSO for (3)H(2)O, (131)IdU, (125)IdU and (210)Po citrate were 2.9 +/- 0.01, 2.3 +/- 0.5, 2.6 +/- 0.2 and 0.95 +/- 0.07, respectively. These results indicate that the toxicity of Auger electron and beta-particle emitters incorporated into the DNA of mammalian cells is largely radical-mediated and is therefore indirect in nature. This is also the case for the low-energy beta particles emitted by (3)H(2)O. In contrast, alpha particles impart lethal damage largely by direct effects. Finally, calculations of cellular absorbed doses indicate that beta-particle emitters are substantially more toxic when incorporated into the DNA of mammalian cells than when they are localized extracellularly.     

Chinese hamster cell mutant resistant to ML236B (Compactin) is defective in endocytosis of low-density lipo-protein.

A fungal metabolite, ML236B (Compactin), isolated from Penicillium citrinum, is a specific inhibitor of 3-hydroxy-3-methylglutaryl (HMG)-coenzyme A reductase (EC 1.1.1.34). Three ML236B-resistant (ML236Br) mutants, MF-1, MF-2, and MF-3, were isolated from V79 after N-methyl-N'-nitro-N-nitrosoguanidine mutagenesis. The fluctuation test showed 2.2 X 10(-6) mutants per cell per generation of a spontaneous mutation frequency of ML236Br clones. These ML236Br clones showed a four- to fivefold-higher resistance to the drug than did their parental V79. Radioactive acetate, but not mevalonate, incorporation into the sterol fraction increased about 10-fold in ML236Br clones in comparison with that in V79. The cellular level of HMG-coenzyme A reductase in three ML236Br mutants was found to be a few-fold higher than that of V79 when cultured in the presence of lipoproteins. The 125I-labeled low-density lipoprotein-binding assay showed binding activity in three ML236Br clones comparable to that of the parental V79 cells. By contrast, an internalization assay of 125I-labeled low-density lipoprotein into the cells showed significantly reduced activity in three ML236Br clones in comparison with V79.     

DNA double-strand break repair in eukaryotic cell lines having radically different radiosensitivities

TN-368 lepidopteran insect cells are on the order of 100 times more resistant to the lethal effects of ionizing radiation than cultured mammalian cells. DNA double-strand breaks (DSB) are believed by many to be the critical molecular lesion leading to cell death. We have therefore compared the rejoining of DSB in TN-368 and V79 Chinese hamster cells. Cells were irradiated on ice with 137Cs gamma rays at a dose rate of 2.5 Gy/min, incubated for various periods of time, and assayed for DNA DSB using the method of neutral elution. The kinetics of DSB rejoining following a dose of 90.2 Gy is similar for both cell lines with 50% of the rejoining completed in about 12 min. Approximately 83 and 87% of the DSB are rejoined in the TN-368 and V79 cells, respectively, by 1 h postirradiation. However, no further rejoining occurs in the TN-368 cells through at least 6 h postirradiation, whereas approximately 92% of the DSB are rejoined in the V79 cells by 2 h postirradiation. Other studies (from 22.6 to 226 Gy) demonstrate that the amount of rejoining of DSB varies inversely with dose for both cell lines, but this relationship is not as pronounced for the TN-368 cells. In general, these findings do not support the hypothesis that unrejoined DNA DSB represent the critical molecular lesion responsible for cell death.     

RBE of 10 kV X rays determined for the human mammary epithelial cell line MCF-12A

The dependence of relative biological effectiveness (RBE) on photon energy is a topic of extensive discussions. The increasing amount of in vitro data in the low-energy region indicates this to be a complex dependence that is influenced by the end point and cell line studied. In the present investigation, the RBE of 10 kV X rays (W anode) was determined relative to 200 kV X rays (W anode, 0.5 mm copper filter) for cell survival in the dose range 1-10 Gy and for induction of micronuclei in the range 0.5-3.6 Gy for MCF-12A human mammary epithelial cells. The RBE for cell survival was found to increase with decreasing dose, being 1.21+/-0.03 at 10% survival. Considerably higher values were obtained for micronucleus induction, where the RBE(M) obtained from the ratio of the linear coefficients of the dose-effect curves was 2.6+/-0.4 for the fraction of binucleated cells with micronuclei and 4.1+/-1.0 for the number of micronuclei per binucleated cell. These values, together with our previous data, support a monotonic increase in RBE with decreasing photon energy down to the mean energy of 7.3 keV used in the present study.     

Enhanced values of the RBE and H ratio for cytogenetic effects induced by secondary electrons from an X-irradiated gold gurface

The low-energy secondary electrons emerging from the entrance surface of an X-irradiated gold foil increase the dose to cells in contact with or at micrometer distances from this surface (Radiat. Res. 150, 92-100, 1998). We examined the effect of the spectrum of these low-energy electrons on the RBE for cytogenetic effects and showed that this RBE was increased. A monolayer of surface-attached human T lymphocytes was exposed to 60 kV X rays in the absence or presence of a gold foil positioned immediately behind the cell layer or separated from it by a Mylar foil 0.9 or 2 microm thick. The enhancement of dose in the cell nuclei caused by the photoelectrons and Auger electrons emerging from the entrance surface of the gold foil was measured by TSEE dosimetry. Dose enhancement factors of 55.7, 46.6 and 37.5 were obtained with 0, 0.9 and 2 microm of Mylar inserted between the gold surface and the cell layer. This large enhancement results from the photoelectric effect in the gold foil, as shown by the accompanying Monte Carlo calculations of the secondary electron spectra at the gold surface. Auger electrons from the gold foil generally were not able to penetrate into the cell nuclei except for that fraction of the cells that had a very thin (< 0.7 microm) layer of cytoplasm and membranes between gold surface and cell nucleus. The dose-yield curves for dicentric chromosomes plus centric rings and for acentric fragments obtained after exposures without or with the gold foil were linear-quadratic. The coefficient alpha, the slope of the linear yield component, was increased in the presence of the gold foil and showed RBE values ranging from 1.7 to 2.2 compared to exposures in absence of the gold foil. The ratio of the yield of interstitial deletions and dicentrics (H ratio) was significantly increased from about 0.17 in the absence of the gold foil to about 0.22 in the presence of the gold foil. The increases in the RBE and the H ratio are interpreted in microdosimetric terms: The preferred occurrence of electron track ends in the vicinity of the gold surface causes an increase in the dose-mean restricted linear energy transfer in cell nuclei exposed to the photoelectrons and Auger electrons.     

125I-induced DNA double strand breaks: use in calibration of the neutral filter elution technique and comparison with X-ray induced breaks

The neutral filter elution assay, for measurement of DNA double strand breakage, has been calibrated using mouse L cells and Chinese hamster V79 cells labelled with [125I]dUrd and then held at liquid nitrogen temperature to accumulate decays. The basis of the calibration is the observation that each 125I decay, occurring in DNA, produces a DNA double strand break. Linear relationships between 125I decays per cell and lethal lesions per cell (minus natural logarithm survival) and the level of elution, were found. Using the calibration data, it was calculated that the yield of DNA double strand breaks after X-irradiation of both cell types was from 6 to 9 X 10(-12) DNA double strand breaks per Gy per dalton of DNA, for doses greater than 6 Gy. Neutral filter elution and survival data for X-irradiated and 125I-labelled cells suggested that the relationships between lethal lesions and DNA double strand breakage were significantly different for both cell types. An attempt was made to study the repair kinetics for 125I-induced DNA double strand breaks, but was frustrated by the rapid DNA degradation which occurs in cells that have been killed by the freezing-thawing process.     

Kinetics of uptake, retention, and radiotoxicity of 125IUdR in mammalian cells: implications of localized energy deposition by Auger processes

The kinetics of uptake, retention, and radiotoxicity of 125IUdR have been studied in proliferating mammalian cells in culture. The radioactivity incorporated into the DNA is directly proportional to the duration of incubation and to the extracellular concentration of 125I. The rate of proliferation of cells is related to the intracellular radioactive concentration and is markedly reduced at medium concentrations greater than or equal to 0.1 mu Ci/ml. At 37% survival the high LET type cell survival curve is characterized by an uptake of 0.035 pCi/cell, and the cumulated mean lethal dose to the cell nucleus is about 80 rad compared to 580 rad of X-ray dose for this cell line. The strong cytocidal effects of the decay of 125I correlate with localized irradiation of the DNA by the low energy Auger electrons.