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PubMed1984

The genotoxicity of alpha particles in human embryonic skin fibroblasts.

Cell inactivation and induced mutation frequencies at the hypoxanthine-guanine phosphoribosyl transferase (HGPRT) locus have been measured in cultured human fibroblasts (GM10) exposed to alpha particles from 238Pu (LET at the cell surface was 100 keV/microns) and 250 kVp X rays. The survival curves resulting from exposure to alpha particles are exponential. The mean lethal dose, D0, is approximately 1.3 Gy for X rays and 0.25 Gy for alpha particles. As a function of radiation dose, mutation induction at the HGPRT locus was linear for alpha particles whereas the X-ray-induced mutation data were better fitted by a quadratic function. When mutation frequencies were plotted against the log of survival, mutation frequency at a given survival level was greater in cells exposed to alpha particles than to X rays.

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PubMed1995

Effects of alpha-particles on survival and chromosomal aberrations in human mammary epithelial cells.

We have studied the radiation responses of a human mammary epithelial cell line, H184B5 F5-1 M/10. This cell line was derived from primary mammary cells after treatment with chemicals and heavy ions. The F5-1 M/10 cells are immortal, density-inhibited in growth, and non-tumorigenic in athymic nude mice and represent an in vitro model of the human epithelium for radiation studies. Because epithelial cells are the target of alpha-particles emitted from radon daughters, we concentrated our studies on the efficiency of alpha-particles. Confluent cultures of M/10 cells were exposed to accelerated alpha-particles [beam energy incident at the cell monolayer = 3.85 MeV, incident linear energy transfer (LET) in cell = 109 keV/microns] and, for comparison, to 80 kVp x-rays. The following endpoints were studied: (1) survival, (2) chromosome aberrations at the first postirradiation mitosis, and (3) chromosome alterations at later passages following irradiation. The survival curve was exponential for alpha-particles (D0 = 0.73 +/- 0.04 Gy), while a shoulder was observed for x-rays (alpha/beta = 2.9 Gy; D0 = 2.5 Gy, extrapolation number 1.6). The relative biological effectiveness (RBE) of high-LET alpha-particles for human epithelial cell killing was 3.3 at 37% survival. Dose-response curves for the induction of chromosome aberrations were linear for alpha-particles and linearquadratic for x-rays. The RBE for the induction of chromosome aberrations varied with the type of aberration scored and was high (about 5) for chromosome breaks and low (about 2) for chromosome exchanges.(ABSTRACT TRUNCATED AT 250 WORDS)

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PubMed1987

Absence of a dose-rate effect in the transformation of C3H 10T1/2 cells by alpha-particles.

The findings of Hill et al. (1984) on the greatly enhanced transformation frequencies at very low dose rates of fission neutrons induced us to perform an analogous study with alpha-particles at comparable dose rates. Transformation frequencies were determined with gamma-rays at high dose rate (0.5 Gy/min), and with alpha-particles at high (0.2 Gy/min) and at low dose rates (0.83-2.5 mGy/min) in the C3H 10T1/2 cell system. alpha-particles were substantially more effective than gamma-rays, both for cell inactivation and for neoplastic transformation at high and low dose rates. The relative biological effectiveness (RBE) for cell inactivation and for neoplastic transformation was of similar magnitude, and ranged from about 3 at an alpha-particle dose of 2 Gy to values of the order of 10 at 0.25 Gy. In contrast to the experiments of Hill et al. (1984) with fission neutrons, no increased transformation frequencies were observed when the alpha-particle dose was protracted over several hours.

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PubMed2000

Oncogenic transformation of mammalian cells by ultrasoft X-rays and alpha particles.

For a better understanding of oncogenic cell transformation by ionizing radiation, we conducted experiments with ultrasoft X rays and low energy alpha particles. Confluent C3H10T1/2 cells were irradiated by Al-K (1.5 keV) X rays or alpha particles from plutonium through a thin mylar sheet, on which the cells attached and grew. Our results indicated that Al-K X rays were more effective in causing cell inactivation and oncogenic transformation than 60Co gamma rays but less effective than 1.0 and 3.7 MeV alpha particles. There was no significant difference between 1.0 and 3.7 MeV alpha particles in transforming cells although the latter were slightly more effective than the former in producing lethal effect. These results indicated that track structure is important in causing biological effects by ionizing radiation.

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PubMed2003

Relative biological effectiveness (RBE) of 210Po alpha-particles versus X-rays on lethality in bovine endothelial cells.

PURPOSE: Alpha-radiation from polonium-210 ((210)Po) can elevate background radiation dose by an order of magnitude in people consuming large quantities of meat and seafood, particularly caribou and reindeer. Because up to 50% of the ingested (210)Po body burden is initially found in the blood, a primary target for the short range alpha-particles is the endothelial cells lining the blood vessels. This study examined the relative biological effectiveness (RBE) of (210)Po alpha-particles versus 250 kVp X-rays in producing injury to cultured bovine aortic endothelial cells. MATERIALS AND METHODS: Radiation effects on cells were measured in four different ways: the percentage viable cells by trypan blue dye exclusion, the number of live cells, the lactate dehydrogenase (LDH) release to medium and the ability to form colonies (clonogenic survival). RESULTS: Comparison of dose-response curves yielded RBE values of 13.1+/-2.5 (SEM) for cell viability, 10.3+/-1.0 for live cell number and 11.1+/-3.0 for LDH activity. The RBE values for clonogenic survival were 14.0+/-1.0 based on the ratio of the initial slopes of the dose-response curves and 13.1, 9.9 and 7.7 for 50, 10 and 1% survival rate, respectively. At X-ray doses <0.25 Gy, a pronounced stimulatory effect on proliferation was noted. CONCLUSIONS: Exposure to (210)Po alpha-particles was seven to 14 times more effective than X-ray exposure in causing endothelial cell damage.

Alpha Particles↗

PubMedDate not supplied

Peak resolution and tailing in alpha-particle spectrometry for environmental samples.

Peak resolution in alpha-particle spectrometry is generally quoted as full-width-at half maximum. However, the extent of tailing of alpha particle peaks into regions of lower energy is often a critical factor for accurate spectral analysis, particularly given the relatively low count rates observed for many environmental samples. In this paper we examine the influence of various factors on peak resolution and tailing for spectra collected using solid-state alpha detectors, in particular chamber gas pressure and source deposit thickness.

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PubMed1988

DNA double-strand break repair determines the RBE of alpha-particles.

Radiation-induced DNA double-strand breaks (dsb) were studied in Ehrlich ascites tumour cells (EATC) by sedimentation in neutral sucrose gradients at low centrifuge speed. Dsb induction was found to be linear with dose with a frequency of: ndsbmr-1D-1 = (11.7 +/- 2) x 10(-12)Gy-1 for 140 kV X-rays and ndsbmr-1D-1 = (19.1 +/- 4) x 10(-12)Gy-1 for 3.4 MeV 241Am-alpha-particles. Postirradiation incubation of cells under non-growth conditions leads to repair of dsb, reaching a maximum after trep = 24 h. More than 97 per cent of dsb were repaired after an X-ray dose of 25 Gy. The number of residual dsb was found to be a linear-quadratic function of dose: nresmr-1 = (0.0161 +/- 0.0008) x 10(-12)Gy-2D2 for X-rays and nresmr-1 = (1.2 +/- 0.7) x 10(-12)Gy-1D + (0.105 +/- 0.017) x 10(-12)Gy-2D2 for alpha-particles. Thus, after cellular repair the RBE value of alpha-particles was increased from RBE = 1.6 +/- 0.4 (induction of dsb) to a dose-dependent value of RBE = 2.7 +/- 0.4 (at 100 Gy alpha-particles) to 3.8 +/- 1.2 (at 10 Gy alpha-particles) for residual dsb. From the data presented it is concluded that residual dsb are a major cause for loss of the reproductive capacity of EATC after irradiation with X-rays as well as alpha-particles.

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PubMed1984

Cell cycle dependent G2 delay and killing of L929 cells after exposure to 241Am alpha particles.

Survival and G2 delay of L929 mouse fibroblasts exposed to 3.4-MeV alpha particles depend on the cell age at the time of irradiation. Greatest sensitivity for both endpoints has been found at the G1/S transition: The surviving fraction of G1/S cells is reduced to 0.11 following 1 Gy of alpha particles compared to 0.31 for early G1 cells. The G2 + M transit time rises from 3 hr for control cells to 22 and 30 hr for cells irradiated with 0.3 Gy in G2 or at the G1/S boundary, respectively. Cells irradiated in early G1 do not show increased G2 + M transit times. Growth delay as calculated for the entire population increases linearly with dose by 23 hr/Gy of alpha particles.

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PubMed1997

DNA double-strand break distributions in X-ray and alpha-particle irradiated V79 cells: evidence for non-random breakage.

Many studies have shown that with increasing LET of ionizing radiation the RBE (relative biological effectiveness) for dsb (double strand breaks) induction remains around 1.0 despite the increase in the RBE for cell killing. This has been attributed to an increase in the complexity of lesions, classified as dsb with current techniques, at multiply damaged sites. This study determines the molecular weight distributions of DNA from Chinese hamster V79 cells irradiated with X-rays or 110 keV/micron alpha-particles. Two running conditions for pulsed-field gel-electrophoresis were chosen to give optimal separation of fragments either in the 225 kbp-5.7 Mbp range or the 0.3 kbp to 225 kbp range. Taking the total fraction of DNA migrating into the gel as a measure of fragmentation, the RBE for dsb induction was less than 1.0 for both molecular weight regions studied. The total yields of dsb were 8.2 x 10(-9) dsb/Gy/bp for X-rays and 7.8 x 10(-9) dsb/Gy/bp for alpha-particles, measured using a random breakage model. Analysis of the RBE of alpha-particles versus molecular weight gave a different response. In the 0.4 Mbp-5.7 Mbp region the RBE was less than 1.0; however, below 0.4 Mbp the RBE increased above 1.0. The frequency distributions of fragment sizes were found to differ from those predicted by a model assuming random breakage along the length of the DNA and the differences were greater for alpha-particles than for X-rays. An excess of fragments induced by a single-hit mechanism was found in the 8-300 kbp region and for X-rays and alpha-particles these corresponded to an extra 0.8 x 10(-9) and 3.4 x 10(-9) dsb/bp/Gy, respectively. Thus for every alpha-particle track that induces a dsb there is a 44% probability of inducing a second break within 300 kbp and for electron tracks the probability is 10%. This study shows that the distribution of damage from a high LET alpha-particle track is significantly different from that observed with low LET X-rays. In particular, it suggests that the fragmentation patterns of irradiated DNA may be related to the higher-order chromatin repeating structures found in intact cells.

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PubMed1996

Alpha particle mutagenesis of human lymphoblastoid cell lines.

Despite being derived from the same donor, the human lymphoblastoid cell lines WTK1 and TK6 have markedly different responses to low LET radiation. We originally observed that WTK1 was more resistant to the cytotoxic effects of X-irradiation, but significantly more sensitive to mutation induction at both the TK and HPRT loci. In an effort to better understand these properties, we have examined the effects of alpha-particles on these cells. Relative to TK6, WTK1 has enhanced survival and mutation after both X-ray and alpha-particle exposure. While the HPRT locus was significantly more mutable in WTK1 as a function of alpha-particle versus X-ray dose, the TK locus was only slightly more sensitive to alpha-particle mutagenesis. In addition, the slowly growing TK mutants that constitute the majority of X-ray-induced TK mutants of TK6 were recovered in lower proportions following alpha-particle exposures. This is consistent with the further finding that in both cell lines, loss of heterozygosity occurred in a smaller fraction of alpha-induced TK mutants than X-ray-induced mutants. These results are consistent with our previous model suggesting that WTK1 has an error-prone repair pathway that is either missing or deficient in TK6, and further suggest that this pathway may be involved in the processing of alpha-particle-induced damage.

Alpha Particles↗

PubMed1987

The effect of 238Pu alpha-particles on the mouse fibroblast cell line C3H 10T1/2: characterization of source and RBE for cell survival.

Considerable interest has been aroused in recent years by reports that the transforming and carcinogenic effectiveness of low doses of high LET radiations can be increased by reducing the dose rate, especially for transformation of 10T1/2 cells in vitro by fission-spectrum neutrons. We report on conditions which have been established for irradiation of 10T1/2 cells with high LET monoenergetic alpha-particles (energy of 3.2 MeV, LET of 124 keV microns-1) from 238Pu. The alpha-particle irradiator allows convenient irradiation of multiple dishes of cells at selectable high or low dose rates and temperatures. The survival curves of irradiated cells showed that the mean lethal dose of alpha-particles was 0.6 Gy and corresponded to an RBE, at high dose rates, of 7.9 at 80 per cent survival and 4.6 at 5 per cent survival, relative to 60Co gamma-rays. The mean areas of the 10T1/2 nuclei, perpendicular to the incident alpha-particles, was measured as 201 microns2, from which it follows that, on average, only one in six of the alpha-particle traversals through a cell nucleus is lethal. Under the well-characterized conditions of these experiments the event frequency of alpha-particle traversals through cell nuclei is 9.8 Gy-1.

Alpha Particles↗

PubMed2003

Quality factors for alpha particles in the human respiratory tract.

Quality factors of alpha particles emitted by radon progeny in the human lung have been calculated by using the formula recommended by the International Commission on Radiological Protection. Calculations have been carried out for different combinations of sources, energies, and targets. The values obtained are between 20 and 26, with an average of about 24. These are comparable to previously published results for the human lung and for the general consideration of alpha particles emitted in tissue.

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PubMed1994

Relative biological effectiveness of alpha-particle emitters in vivo at low doses.

The therapeutic potential of radionuclides that emit alpha particles, as well as their associated health hazards, have attracted considerable attention. The 224Ra daughters 212Pb and 212Bi, by virtue of their radiation properties which involve emission of alpha and beta particles in their decay to stable 208Pb, have been proposed as candidates for radioimmunotherapy. Using mouse testes as the experimental model and testicular spermhead survival as the biological end point, the present work examines the radiotoxicity of 212Pb and its daughters. When 212Pb, in equilibrium with its daughters 212Bi, 212Po and 208Tl, was administered directly into the testis, the dose required to achieve 37% survival (D37) was 0.143 +/- 0.014 Gy and the corresponding RBE of the mixed radiation field was 4.7 when compared to the D37 for acute external 120 kVp X rays. This datum, in conjunction with our earlier results for 210Po, was used to obtain an RBE-LET relationship for alpha particles emitted by tissue-incorporated radionuclides: RBE alpha = 4.8 - 6.1 x 10(-2) LET + 1.0 x 10(-3) LET2. Similarly, the dependence of RBE on alpha-particle energy E alpha was given by RBE alpha = 22 E(-0.73) alpha. These relationships, based on in vivo experimental data, may be valuable in predicting biological effects of alpha-particle emitters.

Alpha Particles↗

PubMed1979

Cell survival following multiple-track alpha particle irradiation.

In experiments in which mammalian cells were irradiated with 5 . 6 MeV alpha particles from a Tandem Van de Graaff machine, we have confirmed the finding of others that the mean lethal dose (Do) is about 60 rad. However, on measuring the area of the nuclei of the flattened cells as they were irradiated, we found that this mean lethal dose corresponds to the passage of not one or two alpha particles per cell nucleus as expected but to between 10 and 20 particles. This allows for the possibility that the direct action of alpha particles on the nucleus may be the important event in carcinogenesis.

Alpha Particles↗

PubMed1989

Breakage of human interphase chromosomes by alpha particles and X-rays.

The technique of premature chromosome condensation (PCC) was used to compare the early formation of chromosome breaks in non-cycling HF19 human diploid fibroblasts when irradiated with slow alpha particles (3.2 MeV, 128 keV micron-1) or 250 kVP X-rays. For both radiations the production of PCC breaks increased approximately linearly with dose. The production coefficient for alpha particles was 12.5 +/- 0.6 per cent per Gy and for X-rays it was 5.8 +/- 0.2 per cell per Gy. Hence, the relative biological effectiveness (RBE) of the alpha particles was 2.16 +/- 0.13. This is smaller than reported values of the RBE for the production of chromosome-type exchange aberrations by slow alpha particles. This implies that there is a difference, spatial or qualitative, in the initial breaks produced by the densely ionizing alpha particle tracks and the more sparsely ionizing electron tracks from the X-rays.

Alpha Particles↗

PubMed1999

Chromosome aberrations induced in human lymphocytes by 3.45 MeV alpha particles analyzed by premature chromosome condensation.

Premature chromosome condensation (PCC) experiments using human lymphocytes with centromere staining have shown that after exposure to 3.45 MeV alpha-particle radiation, the full number of dicentric chromosomes appears when the cell fusion protocol is applied immediately after irradiation. In this case, the time available for repair and misrepair of DNA damage is only about 30 min. The number of dicentrics does not change with a further increase in the time available for chromatin rearrangement. This fast response confirms the expectation based on our previous experiments using PCC with 150 kV X rays in which the alpha component of the yield of dicentrics was found to appear when the cell fusion protocol was applied immediately after irradiation, whereas the beta component was delayed by several hours. The time constant for rejoining of the excess acentric chromosome fragments is found to be donor-specific and not to differ for alpha particles and X rays, but alpha-particle radiation leaves a larger fraction of the excess acentric fragments unrejoined. The RBEs of the 3.45 MeV alpha-particle radiation compared to 150 kV X rays, evaluated for the alpha component for the yield of dicentrics and for the yield of unrepaired acentric fragments, have almost equal values of about 4. This is consistent with data in the literature on chromosome aberrations observed in metaphase that show the equality of the RBE values for production of dicentrics and acentric fragments. Our experimental results concerning the fast kinetics of the alpha component of the yield of exchange-type chromosome aberrations are not consistent with Lea's pairwise lesion interaction model, and they support the proposed alternative mechanism of lesion-nonlesion interaction between chromatin regions carrying clustered DNA damage and intact chromatin regions.

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PubMed1997

Inactivation of individual mammalian cells by single alpha-particles.

PURPOSE: To measure clonogenic death of Chinese hamster V79 cells following exposure to a defined number of 4.3 MeV alpha-particles (track-averaged LET = 105 keV/micron). MATERIALS AND METHODS: Cells were irradiated at the radiobiological facility installed at the TTT-3 Tandem accelerator in Naples by using a 'Biostack' approach, which allows the positions of incident tracks relative to cells to be carefully determined. Subcellular structure was identified by fluorescence microscopy, while tracks were visualized by LR-115 solid state nuclear track detectors. RESULTS: Particle hits in the cytoplasm did not significantly affect cell survival, yet survival probability decreased exponentially as a function of the number of nuclear traversals. Measured probability of surviving to exactly one 4.3 MeV alpha-particle traversal in the cell nucleus was 0.67 +/- 0.10. Inactivation cross-section was substantially higher than expected from conventional survival curves. However, folding of the data with Poisson statistics showed that survival level expected if a mean of one alpha-particle goes through a nucleus is higher than the measured value after exactly one particle traversal. CONCLUSIONS: V79 cells have about 67% probability to survive a single alpha-particle traversal in the cell nucleus. Single-particle survival curves are consistent with conventional dose-survival relationships, once Poisson distribution of traversals is taken into account.

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PubMed2004

First gamma-ray measurements of fusion alpha particles in JET trace tritium experiments.

Gamma-ray spectra from nuclear reactions between fusion-born alpha (alpha) particles and Be impurities were measured for the first time in deuterium-tritium plasmas in the Joint European Torus. The time dependence of the measured spectra allowed the determination of the density evolution of fast alpha particles. Correlation between the decay time of the gamma-ray emission and the plasma parameters in different plasma scenarios was established. Results are consistent with classical slowing down of the alpha particles in discharges with high plasma currents and monotonic q-profiles. In low plasma current discharges and in the discharges with large on-axis current holes (extreme reversal central magnetic shear), the gamma-ray emission decay times are shorter than the classical slowing down times, indicating an alpha-particle confinement degradation in such discharges in line with theoretical predictions.

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