Clonal heterogeneity in delayed decrease of plating efficiency of irradiated HeLa cells

The clonogenic potential of progeny of irradiated HeLa cells was studied at different times after single doses of 4–12 Gy. The dose-dependent decrease in plating efficiency that was observed resembled the effect termed delayed lethal mutation by Seymour et al. (1986). The effect decreased with time after irradiation. Individual clones of irradiated and non-irradiated cells were isolated, expanded and replated 5 weeks after irradiation, i.e., after between 200000 and 1000 000 progeny had formed from the individual parent cell. The plating efficiency of progeny of unirradiated cells did not vary much, whereas clonal progeny of irradiated cells had plating efficiencies ranging from 3% to 76%. The plating efficiency was not related to the cell number in the original clone.     

Ionizing Irradiation Not Only Inactivates Clonogenic Potential in Primary Normal Human Diploid Lens Epithelial Cells but Also Stimulates Cell Proliferation in a Subset of This Population

Over the past century, ionizing radiation has been known to induce cataracts in the crystalline lens of the eye, but its mechanistic underpinnings remain incompletely understood. This study is the first to report the clonogenic survival of irradiated primary normal human lens epithelial cells and stimulation of its proliferation. Here we used two primary normal human cell strains: HLEC1 lens epithelial cells and WI-38 lung fibroblasts. Both strains were diploid, and a replicative lifespan was shorter in HLEC1 cells. The colony formation assay demonstrated that the clonogenic survival of both strains decreases similarly with increasing doses of X-rays. A difference in the survival between two strains was actually insignificant, although HLEC1 cells had the lower plating efficiency. This indicates that the same dose inactivates the same fraction of clonogenic cells in both strains. Intriguingly, irradiation enlarged the size of clonogenic colonies arising from HLEC1 cells in marked contrast to those from WI-38 cells. Such enhanced proliferation of clonogenic HLEC1 cells was significant at ≥2 Gy, and manifested as increments of ≤2.6 population doublings besides sham-irradiated controls. These results suggest that irradiation of HLEC1 cells not only inactivates clonogenic potential but also stimulates proliferation of surviving uniactivated clonogenic cells. Given that the lens is a closed system, the stimulated proliferation of lens epithelial cells may not be a homeostatic mechanism to compensate for their cell loss, but rather should be regarded as abnormal. This is because these findings are consistent with the early in vivo evidence documenting that irradiation induces excessive proliferation of rabbit lens epithelial cells and that suppression of lens epithelial cell divisions inhibits radiation cataractogenesis in frogs and rats. Thus, our in vitro model will be useful to evaluate the excessive proliferation of primary normal human lens epithelial cells that may underlie radiation cataractogenesis, warranting further investigations.     

The proliferative capacity of mouse fibrosarcoma cells that survived x-irradiation

Delayed reproductive death, the appearance of colonies with a reduced cell density (impaired colonies) and the number of giant cells per colony were investigated in murine fibrosarcoma cells after irradiation with 3 to 9 Gy of x-rays. Radiation survivors were replated after reaching confluence, which occurred after 13 to 15 doublings; this procedure was repeated three times. The replating efficiency decreased in a dose-dependent manner, the survivors of 9 Gy achieving only 30% of the plating efficiency of unirradiated cells. After the third replating, i.e. after 40 to 45 doublings, the plating efficiency of the survivors approached that of the controls. The median colony size of the survivors showed a similar dose-dependent decrease, which was pronounced after the first replating but still remained significant after the third replating. The fraction of impaired colonies was increased to more than 30% in 9-Gy survivors, and though abating, the increase was still significant even after the third replating. Evidence of residual damage was also provided by the presence of giant cells. For instance, after 6 Gy irradiation and 13 to 15 doublings, the proportion of colonies with giant cells was 60%, decreasing only to 45% after 40 to 45 doublings. The number of giant cells per colony was 1.4 in colonies arising immediately after 6 Gy, decreasing to 0.9 after the third replating. These results suggest that the proliferative capacity of surviving cells is depressed even longer than their clonogenic capacity.     

The generation and characterization of a radiation-resistant model system to study radioresistance in human breast cancer cells.

To systematically study the selection of radioresistant cells in clinically advanced breast cancer, a model system was generated by treating MDA-MB231 breast cancer cells with fractionated gamma radiation. A clonogenic assay of the surviving cell populations showed that 2-6 Gy per fraction resulted in a rapid selection of radioresistant populations, within three to five fractions. Irradiation with additional fractions after this initial increase did not increase the radioresistance of the surviving population significantly. Doses of 0.5 and 8 Gy per fraction were not effective in selecting radioresistant cells. To further determine the cause of the changes in radiosensitivity, 15 clones were isolated from the cell populations treated with 40 or 60 Gy with 2 or 4 Gy per fraction, respectively, and were analyzed for radiosensitivity. The average D(10) for these clones was 6.75 +/- 0.36 Gy, which was higher than that for the parental cell population (D(10) = 6.0 +/- 0.2 Gy). The operation of cell cycle checkpoints and the doubling time were similar for both the nonirradiated parental population and the isolated radioresistant subclones. In contrast, a decrease in the apoptotic potential was correlated (r = 0.7, P < 0.01) with increased survival after irradiation, suggesting that apoptosis is an important factor in determining radioresistance under our experimental conditions. We also isolated several subclones from the nonirradiated parental cell population and analyzed them to determine their radiosensitivity after fractionated irradiation. Ten fractions of 4 Gy (40 Gy in total) did not result in a significant increase in the radioresistance of these subclones compared to the irradiated cell populations. The possible mechanisms of the increased radioresistance after fractionated irradiation are discussed.     

Isolation and characterization of highly radioresistant malignant hamster fibroblasts that survive acute gamma irradiation with 20 Gy

To study the acquired radioresistance of tumor cells, a model system of two cell lines, Djungarian hamster fibroblasts (DH-TK-) and their radioresistant progeny, was established. The progeny of irradiated cells were isolated by treating the parental cell monolayer with a single dose of 20 Gy (PIC-20). The genetic and morphological features, clonogenic ability, radiosensitivity, cell growth kinetics, ability to grow in methylcellulose, and tumorigenicity of these cell lines were compared. The plating efficiency of PIC-20 cells exceeded that of DH-TK- cells. The progeny of irradiated cells were more radioresistant than parental cells. The average D0 for PIC-20 cells was 7.4 +/- 0.2 Gy, which is three times higher than that for parental cells (2.5 +/- 0.1 Gy). Progeny cell survival in methylcellulose after irradiation with a dose of 10 Gy was 15 times higher than that of DH-TK- cells. In contrast to parental cells, the progeny of irradiated cells showed fast and effective repopulation after irradiation with doses of 12.5 and 15 Gy. The tumor formation ability of irradiated progeny cells was higher than that of parental cells; after 15 Gy irradiation, PIC-20 cells produced tumors as large as unirradiated progeny of irradiated cells, whereas the tumor development of DH-TK- cells diminished by 70%. High radioresistance of progeny of irradiated cells was reproduced during the long period of cultivation (more than 80 passages). The stability of the radioresistant phenotype of PIC-20 cells allows us to investigate the possible mechanisms of acquired tumor radioresistance.     

Computerized video time-lapse analysis of apoptosis of REC:Myc cells X-irradiated in different phases of the cell cycle

Asynchronous rat embryo cells expressing Myc were followed in 50 fields by computerized video time lapse (CVTL) for three to four cycles before irradiation (4 Gy) and then for 6-7 days thereafter. Pedigrees were constructed for single cells that had been irradiated in different parts of the cycle, i.e. at different times after they were born. Over 95% of the cell death occurred by postmitotic apoptosis after the cells and their progeny had divided from one to six times. The duration of the process of apoptosis once it was initiated was independent of the phase in which the cell was irradiated. Cell death was defined as cessation of movement, typically 20-60 min after the cell rounded with membrane blebbing, but membrane rupture did not occur until 5 to 40 h later. The times to apoptosis and the number of divisions after irradiation were less for cells irradiated late in the cycle. Cells irradiated in G(1) phase divided one to six times and survived 40-120 h before undergoing apoptosis compared to only one to two times and 5-40 h for cells irradiated in G(2) phase. The only cells that died without dividing after irradiation were irradiated in mid to late S phase. Essentially the same results were observed for a dose of 9.5 Gy, although the progeny died sooner and after fewer divisions than after 4 Gy. Regardless of the phase in which they were irradiated, the cells underwent apoptosis from 2 to 150 h after their last division. Therefore, the postmitotic apoptosis did not occur in a predictable or programmed manner, although apoptosis was associated with lengthening of both the generation time and the duration of mitosis immediately prior to the death of the daughter cells. After the non-clonogenic cells divided and yielded progeny entering the first generation after irradiation with 4 Gy, 60% of the progeny either had micronuclei or were sisters of cells that had micronuclei, compared to none of the progeny of clonogenic cells having micronuclei in generation 1. However, another 20% of the non-clonogenic cells had progeny with micronuclei appearing first in generation 2 or 3. As a result, 80% of the non-clonogenic cells had progeny with micronuclei. Furthermore, cells with micronuclei were more likely to die during the generation in which the micronuclei were observed than cells not having micronuclei. Also, micronuclei were occasionally observed in the progeny from clonogenic cells in later generations at about the same time that lethal sectoring was observed. Thus cell death was associated with formation of micronuclei. Most importantly, cells irradiated in late S or G(2) phase were more radiosensitive than cells irradiated in G(1) phase for both loss of clonogenic survival and the time of death and number of divisions completed after irradiation. Finally, the cumulative percentage of apoptosis scored in whole populations of asynchronous or synchronous populations, without distinguishing between the progeny of individually irradiated cells, underestimates the true amount of apoptosis that occurs in cells that undergo postmitotic apoptosis after irradiation. Scoring cell death in whole populations of cells gives erroneous results since both clonogenic and non-clonogenic cells are dividing as non-clonogenic cells are undergoing apoptosis over a period of many days.     

Repopulation kinetics of rat rhabdomyosarcoma tumors following single and fractionated doses of low-LET and high-LET radiation

Measurements were made of clonogenic cell survival in rat rhabdomyosarcoma tumors as a function of time following in situ irradiation with single or fractionated doses of 225-kVp X rays or with 557-MeV/u neon ions in the distal position of a 4-cm extended-peak ionization region. Single doses of 20 Gy of X rays or 7 Gy of peak neon ions reduced the initial surviving fraction to approximately 0.025 for each modality. Daily fractionated doses (four fractions in 3 days) of either peak neon ions (1.75 Gy per fraction) or X rays (6 Gy per fraction) achieved a cell survival of approximately 0.02-0.03 after the fourth dose of radiation. In the single-dose experiments, significant 5- and 10-fold decreases in the fraction of clonogenic cells were observed between the third and fourth days after irradiation with peak neon ions and X rays, respectively. After the sixth day postirradiation, the residual clonogenic cells exhibited a rapid burst of proliferation leading to doubling times for the surviving cell fractions of approximately 1.5 days. Radiation-induced growth delay was consistent with the cellular repopulation dynamics. In the fractionated-dose experiments with both radiation modalities, a large delayed decrease in cell survival was observed at 1-3 days after completion of the fractionated-dose schedule. Cellular repopulation was consistent with postirradiation tumor volume regression and regrowth for both radiation modalities. The extent of decrease in survival following the four-fraction radiation schedule was approximately two times greater in X-irradiated than in neon-ion-irradiated tumors that produced the same survival level immediately after the fourth dose. Mechanisms underlying the marked reduction in cell survival 3-4 days postirradiation are discussed, including the possible role of a toxic host cell response against the irradiated tumor cells.     

A clonogenic survival assay of neural stem cells in rat spinal cord after exposure to ionizing radiation

Neural stem cells play an important role in neurogenesis of the adult central nervous system (CNS). Inhibition of neurogenesis has been suggested to be an underlying mechanism of radiation-induced CNS damage. Here we developed an in vivo/ in vitro clonogenic assay to characterize the survival of neural stem cells after exposure to ionizing radiation. Cells were isolated from the rat cervical spinal cord and plated as single cell suspensions in defined medium containing epidermal growth factor and basic fibroblast growth factor. The survival of the proliferating cells was determined by their ability to form neurosphere colonies. The number and size of neurospheres were analyzed quantitatively at day 10, 12, 14 and 16 after plating. Plating cells from 5, 10 and 15 mm of the cervical spinal cord resulted in a linear increase in the number of neurospheres from day 10-16. Compared to the nonirradiated spinal cord, there was a significant decrease in the number and size of neurosphere colonies cultured from a 10-mm length of the rat spinal cord after a single dose of 5 Gy. When dissociated neurospheres derived from a spinal cord that had been irradiated with 5 Gy were allowed to differentiate, the percentages of neurons, oligodendrocytes and astrocytes as determined by immunocytohistochemistry were not altered compared to those from the nonirradiated spinal cord. Secondary neurospheres could be obtained from cells dissociated from primary neurospheres that had been cultured from the irradiated spinal cord. In conclusion, exposure to ionizing radiation reduces the clonogenic survival of neural stem cells cultured from the rat spinal cord. However, neural stem cells retain their pluripotent and self-renewing properties after irradiation. A neurosphere-based assay may provide a quantitative measure of the clonogenic survival of neural stem cells in the adult CNS after irradiation.     

Delayed chromosomal instability induced by DNA damage.

DNA damage induced by ionizing radiation can result in gene mutation, gene amplification, chromosome rearrangements, cellular transformation, and cell death. Although many of these changes may be induced directly by the radiation, there is accumulating evidence for delayed genomic instability following X-ray exposure. We have investigated this phenomenon by studying delayed chromosomal instability in a hamster-human hybrid cell line by means of fluorescence in situ hybridization. We examined populations of metaphase cells several generations after expanding single-cell colonies that had survived 5 or 10 Gy of X rays. Delayed chromosomal instability, manifested as multiple rearrangements of human chromosome 4 in a background of hamster chromosomes, was observed in 29% of colonies surviving 5 Gy and in 62% of colonies surviving 10 Gy. A correlation of delayed chromosomal instability with delayed reproductive cell death, manifested as reduced plating efficiency in surviving clones, suggests a role for chromosome rearrangements in cytotoxicity. There were small differences in chromosome destabilization and plating efficiencies between cells irradiated with 5 or 10 Gy of X rays after a previous exposure to 10 Gy and cells irradiated only once. Cell clones showing delayed chromosomal instability had normal frequencies of sister chromatid exchange formation, indicating that at this cytogenetic endpoint the chromosomal instability was not apparent. The types of chromosomal rearrangements observed suggest that chromosome fusion, followed by bridge breakage and refusion, contributes to the observed delayed chromosomal instability.     

Bystander and delayed effects after fractionated radiation exposure

Human immortalized keratinocytes were exposed to a range of single or fractionated doses of gamma rays from (60)Co, to medium harvested from donor cells exposed to these protocols, or to a combination of radiation and irradiated cell conditioned medium (ICCM). The surviving fractions after direct irradiation or exposure to ICCM were determined using a clonogenic assay. The results show that medium harvested from cultures receiving fractionated irradiation gave lower "recovery factors" than direct fractionated irradiation, where normal split-dose recovery occurred. The recovery factor is defined here as the surviving fraction of the cells receiving two doses (direct or ICCM) separated by an interval of 2 h divided by the surviving fraction of cells receiving the same dose in one exposure. After treatment with ICCM, the recovery factors were less than 1 over a range of total doses from 5 mGy-5 Gy. Varying the time between doses from 10 min to 180 min did not alter the effect of ICCM, suggesting that two exposures to ICCM are more toxic than one irrespective of the dose used to generate the response. In certain protocols using mixtures of direct irradiation and ICCM, it was possible to eliminate the bystander effect. If bystander factors are produced in vivo, then they may reduce the sparing effect of the dose fractionation.     

Effect of keratinocyte growth factor on radiation survival and colony size of human epidermal keratinocytes in vitro.

Keratinocyte growth factor (FGF7, also known as KGF) ameliorates the radiation response of mouse oral mucosa and other epithelial tissues. However, the precise mechanisms remain unclear. The aim of the present study was to investigate the effect of FGF7 on the survival and colony size of normal human epidermal keratinocytes in vitro. Primary neonatal keratinocytes (HEKn) were irradiated with doses of 0 and 2 Gy of 200 kV X rays and incubated in the presence or absence of 100 ng/ml FGF7. The plating efficiency (PE) and surviving fraction (SF2) were determined using a clonogenic assay. In cell cultures without FGF7, the mean PE was 4.6 +/- 0.2%. Irradiation with 2 Gy resulted in an SF2 of 51 +/- 2%. In cell cultures with FGF7, the mean PE was identical, and a similar SF2 of 54 +/- 1% was observed (P = 0.4). However, the individual colony size was significantly increased in all cultures incubated with FGF7 compared to those incubated without FGF7. The number of extremely large colonies (> or =2 mm) was clearly higher (P < 0.0001) in cultures with FGF7. This was accompanied by a significant reduction in the diameter of individual cells from 29 microm in controls to 23 microm with FGF7. In conclusion, FGF7 does not affect the survival of keratinocytes after irradiation, but it does stimulate proliferation of surviving cells.     

Plating efficiency as a function of time postirradiation: evidence for the delayed expression of lethal mutations

The plating efficiency (PE) of a gamma-irradiated (7 Gy) human cell hybrid line (HeLa X skin fibroblast, designated as CGL1) has been measured as a function of time postirradiation and compared to that of unirradiated cells at similar cell densities and under the same growth conditions. The results indicate that following irradiation, the PE of the irradiated cells initially increases but never returns to that of unirradiated cells during the experimental period that we have examined. Furthermore, after a period of 9 to 10 days (equivalent to at least 10 cell doublings) postirradiation and plating, the PE of the irradiated cells begins to decrease and continues to do so over the next 5 days. A decrease does not occur in unirradiated cells until much later (i.e., Day 15) corresponding to at least 5 additional cell doublings. The data are discussed in terms of a delayed expression of lethal mutations. The possible impact of these observations on the estimation of radiation-induced transformation frequencies is also considered.     

Bystander-mediated genomic instability after high LET radiation in murine primary haemopoietic stem cells

Communication between irradiated and unirradiated (bystander) cells can result in responses in unirradiated cells that are similar to responses in their irradiated counterparts. The purpose of the current experiment was to test the hypothesis that bystander responses will be similarly induced in primary murine stem cells under different cell culture conditions. The experimental systems used here, co-culture and media transfer, are similar in that they both restrict communication between irradiated and bystander cells to media borne factors, but are distinct in that with the media transfer technique, cells can only communicate after irradiation, and with co-culture, cells can communication before, during and after irradiation. In this set of parallel experiments, cell type, biological endpoint, and radiation quality and dose, were kept constant. In both experimental systems, clonogenic survival was significantly decreased in all groups, whether irradiated or bystander, suggesting a substantial contribution of bystander effects (BE) to cell killing. Genomic instability (GI) was induced under all radiation and bystander conditions in both experiments, including a situation where unirradiated cells were incubated with media that had been conditioned for 24h with irradiated cells. The appearance of delayed aberrations (genomic instability) 10-13 population doublings after irradiation was similar to the level of initial chromosomal damage, suggesting that the bystander factor is able to induce chromosomal alterations soon after irradiation. Whether these early alterations are related to those observed at later timepoints remains unknown. These results suggest that genomic instability may be significantly induced in a bystander cell population whether or not cells communicate during irradiation.     

Host cell cytotoxicity, cellular repopulation dynamics, and phase-specific cell survival in X-irradiated rat rhabdomyosarcoma tumors

Postirradiation tumor volume response, cellular repopulation dynamics, cell-cycle perturbations, and phase-specific cell survival were characterized in rat rhabdomyosarcoma R-1 tumors (the R2C5 subline) following an in situ 10-Gy dose of 225-kVp X rays. This X-ray dose produced a 7.5-day delay in tumor growth to twice the volume measured at the time of irradiation, and reduced the initial surviving fraction of R2C5 cells to 0.17 as measured by the excision assay procedure. The surviving fraction of R2C5 cells returned to unity by the 16th day after tumor irradiation. On the basis of flow cytometry measurements of DNA content in tumor cells stained with a noncytotoxic concentration of Hoechst 33342 (5 microM, 2 h, 37 degrees C), a transient G2 block was observed 1 day after irradiation. Flow cytometry measurements also demonstrated that the tetraploid R2C5 cells constituted only 30% of the total tumor cell population, with the remainder being diploid host cells comprised of macrophages, monocytes, lymphocytes, and granulocytes. Large numbers of host cells infiltrated the irradiated tumors, leading to an increase in the percentage of diploid cells by Day 2 and reaching a level of more than 80% of the total tumor cell population by 4 to 8 days after irradiation. The influx of host cells into irradiated tumors was correlated temporally with a significant 12-fold decrease in the surviving fraction of R2C5 cells that occurred between Days 2 and 4 postirradiation. When the diploid host cell population was removed by cell sorting procedures, the surviving fraction of R2C5 cells at Day 4 was substantially greater than that in the presence of the host cells. Experiments involving the mixing of 4/1 and 12/1 ratios of diploid host cells and tetraploid tumor cells isolated from irradiated and unirradiated tumors demonstrated that the cytotoxic effect of the host cells was specific for the irradiated tumor cells. The significant toxic effect of host cells on irradiated tumor cells was observed only at 2 to 4 days after irradiation, and not at earlier or later times. The data obtained in these experiments indicate that the immunogenicity of R2C5 cells is increased significantly by irradiation, and a resultant cell-mediated host immune response produced a delayed decrease in tumor cell survival that is most pronounced 4 days after irradiation. The cell survival characteristics of R2C5 cells in different cell-cycle phases were found to be similar through the 16-day postirradiation interval that was studied.(ABSTRACT TRUNCATED AT 250 WORDS)     

Response of human squamous cell carcinoma xenografts of different sizes to irradiation: relationship of clonogenic cells, cellular radiation sensitivity in vivo, and tumor rescuing units

The relationship of clonogenic cells, cellular radiation sensitivity at tumor control does in vivo, and tumor rescuing units at different tumor sizes was investigated in the human squamous cell carcinoma FaDu growing in NCr/Sed nude mice. The composition of the tumors was determined in single cell suspensions and compared to tumor control data after single-dose irradiation. To avoid the influence of varying oxygen concentrations in the tumors, all irradiations were performed under clamp hypoxia. Nude mice and animals further immunosuppressed by 6-Gy whole-body irradiation were used to assess the immunological effects. The numbers of total cells, cells excluding trypan blue, host cells, and colony-forming cells increased linearly with the weight of FaDu tumors. Comparable results were obtained for cell suspensions prepared from tumors growing in nude of pretreated nude mice. The radiation dose required to control 50% of tumors (TCD50) of different sizes between 36 and 470 mm3 increased from 52.1 to 60.1 Gy when the tumors were maintained in normal nude mice and from 50.8 to 61.3 Gy in whole-body-irradiated mice. The D0 of FaDu cells in vivo was calculated by regression analysis of TCD50 vs the logarithm of the clonogenic cell number, assuming an oxygen enhancement ratio of 3.0. The resultant D0S of 1.1 and 1.2 Gy in vivo correspond well to the radiosensitivity of FaDu cells in vitro determined previously. Assuming the single-hit multitarget model of cell killing and extrapolation numbers between 2 and 20, the mean number of tumor rescuing units would be 10(5) to 10(6) for a 100-mm3 tumor growing in whole-body-irradiated nude mice. Comparison of the number of tumor rescuing units to the estimated number of clonogenic cells does not conflict with the assumption that every surviving clonogenic cell is able to repopulate FaDu tumors after irradiation; however, it seems more likely that more than one clonogenic cells is necessary. The proportion of tumor rescuing units in the clonogenic cell population is independent of tumor size.     

The Growth of the Emt6 Tumour In the Lungs of Balb C Mice Following Intravenous Inoculation of Tumour Cells From Culture

The growth of the EMT6 tumour in the lungs of Balb C mice has been studied following intravenous inoculation of different numbers of tumour cells taken from culture. At various times after injection of cells into mice, cell suspensions have been prepared from pairs of lungs and the number of in vitro colony forming cells assayed by plating into petri dishes. Following intravenous injection of 10⁵ cells, the time required for doubling of the number of clonogenic tumour cells appearing in the cell suspension is around 17 hr until such time that the total tumour cell population per set of lungs reaches 10⁸ cells (at 10–12 days). This doubling time has to be corrected for changes in ability to extract cells from the lungs into the cell suspension at various times and also for possible changes in plating efficiency in vitro. When these correction factors are applied, the most likely value for the doubling time of clonogenic tumour cells in the lungs is in the range 20–24 hr. This is a similar figure to that previously deduced for the EMT6 flank tumour during its microscopic period of growth. After reaching a total size of 10⁸ tumour cells, the time for doubling of the number of clonogenic tumour cells in the lung increases. During the later stages of tumour growth a good correlation is seen between total lung tumour weight and the number of clonogenic cells present. For the final 3–4 days of the initial period of rapid tumour growth, it is possible to carry out a haemocytometer count of tumour cells in the lung suspension and hence surviving fraction experiments may be carried out after various forms of treatment. In this way the response to treatment of microscopic tumour foci may be determined.     

Decay of γ-H2AX foci correlates with potentially lethal damage repair and P53 status in human colorectal carcinoma cells

The influence of p53 status on potentially lethal damage repair (PLDR) and DNA double-strand break (DSB) repair was studied in two isogenic human colorectal carcinoma cell lines: RKO (p53 wild-type) and RC10.1 (p53 null). They were treated with different doses of ionizing radiation, and survival and the induction of DNA-DSB were studied. PLDR was determined by using clonogenic assays and then comparing the survival of cells plated immediately with the survival of cells plated 24 h after irradiation. Doses varied from 0 to 8 Gy. Survival curves were analyzed using the linear-quadratic formula: S(D)/S(0) = exp-(αD+βD²). The γ-H2AX foci assay was used to study DNA DSB kinetics. Cells were irradiated with single doses of 0, 0.5, 1 and 2 Gy. Foci levels were studied in non-irradiated control cells and 30 min and 24 h after irradiation. Irradiation was performed with gamma rays from a ¹³⁷Cs source, with a dose rate of 0.5 Gy/min. The RKO cells show higher survival rates after delayed plating than after immediate plating, while no such difference was found for the RC10.1 cells. Functional p53 seems to be a relevant characteristic regarding PLDR for cell survival. Decay of γ-H2AX foci after exposure to ionizing radiation is associated with DSB repair. More residual foci are observed in RC10.1 than in RKO, indicating that decay of γ-H2AX foci correlates with p53 functionality and PLDR in RKO cells.     

Production of delayed death and neoplastic transformation in CGL1 cells by radiation-induced bystander effects

Other investigators have demonstrated by transfer of medium from irradiated cells and by irradiation with low-fluence alpha particles or microbeams that cells do not have to be directly exposed to ionizing radiation to be detrimentally affected, i.e. bystander effects. In this study, we demonstrate by transfer of medium from X-irradiated human CGL1 hybrid cells that the killing of bystander cells reduces the plating efficiency of the nonirradiated CGL1 cells by 33 +/- 6%. In addition, we show that the amount of cell death induced by bystander effects is not dependent on X-ray dose, and that the induction of apoptosis does not appear to be responsible for the cell death. Furthermore, we found that the reduction in plating efficiency in bystander cells is evident for over 18 days, or 22 cell population doublings, after medium transfer, despite repeated refeeding of the cell cultures. Finally, we report the novel observation that bystander effects induced by the transfer of medium from irradiated cells can induce neoplastic transformation. Exposing unirradiated CGL1 cells to medium from cells irradiated with 5 or 7 Gy increased the frequency of neoplastic transformation significantly from 6.3 x 10(-6) in unirradiated controls to 2.3 x 10(-5) (a factor of nearly four). We conclude that the bystander effect induces persistent, long-term, transmissible changes in the progeny of CGL1 cells that result in delayed death and neoplastic transformation. The data suggest that neoplastic transformation in bystander cells may play a significant role in radiation-induced neoplastic transformation at lower doses of X rays.     

Radiosensitizing effect of hyperfractionated radiation

To determine whether hyperfractionated treatment has benefits in the radiation therapy, two melanoma cell lines were irradiated with eight 0.5 Gy fractions as well as one single 4 Gy in vitro. The radiation was performed in air and in hypoxia as well. Cells were also irradiated in the presence of dibromodulcitol, a bifunctional alkylating agent with a weak radiosensitizer effect. The aim of the study was to examine whether hyperfractionation can influence the radiosensitizing effect of the bioreductive agent. Survival of the cells was determined immediately and 24 hours after various treatments by cell counting in hemocytometer and clonogenic assay. The number of the apoptotic cells was determined by the TUNEL assay and was followed up to 72 hours after treatment. Hypoxic cells had higher sensitivity than normoxic cells after 0.5 Gy irradiation. Radiosensitizing enhancement of DBD was higher with fractionated irradiation. The number of the apoptotic cells was significantly higher after hyperfractionated treatments than after single dose treatment combinations. Our results showed the significance of the hyperfractionated irradiation with 0.5 Gy per fraction in vitro.     

Temporally distinct response of irradiated normal human fibroblasts and their bystander cells to energetic heavy ions

Ionizing radiation-induced bystander effects have been documented for a multitude of endpoints such as mutations, chromosome aberrations and cell death, which arise in nonirradiated bystander cells having received signals from directly irradiated cells; however, energetic heavy ion-induced bystander response is incompletely characterized. To address this, we employed precise microbeams of carbon and neon ions for targeting only a very small fraction of cells in confluent fibroblast cultures. Conventional broadfield irradiation was conducted in parallel to see the effects in irradiated cells. Exposure of 0.00026% of cells led to nearly 10% reductions in the clonogenic survival and twofold rises in the apoptotic incidence regardless of ion species. Whilst apoptotic frequency increased with time up to 72 h postirradiation in irradiated cells, its frequency escalated up to 24h postirradiation but declined at 48 h postirradiation in bystander cells, indicating that bystander cells exhibit transient commitment to apoptosis. Carbon- and neon-ion microbeam irradiation similarly caused almost twofold increments in the levels of serine 15-phosphorylated p53 proteins, irrespective of whether 0.00026, 0.0013 or 0.0066% of cells were targeted. Whereas the levels of phosphorylated p53 were elevated and remained unchanged at 2h and 6h postirradiation in irradiated cells, its levels rose at 6h postirradiation but not at 2h postirradiation in bystander cells, suggesting that bystander cells manifest delayed p53 phosphorylation. Collectively, our results indicate that heavy ions inactivate clonogenic potential of bystander cells, and that the time course of the response to heavy ions differs between irradiated and bystander cells. These induced bystander responses could be a defensive mechanism that minimizes further expansion of aberrant cells.