Plutonium particle size determination using an alpha-particle imaging system.
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Aerosols↗
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Yields of SSB and DSB induced in DNA by Al(K) ultrasoft X-rays and alpha-particles: comparison of experimental and simulated yields.
PURPOSE: To compare experimental yields of single strand breaks (SSB) and double strand breaks (DSB) induced in plasmid DNA in aqueous solution by alpha-particles and Al(K) ultrasoft X-rays (USX) with the corresponding yields, generated via computer simulations, for a range of mean diffusion distances of the hydroxyl radical (*OH). MATERIALS AND METHODS: Aerobic, aqueous solutions of plasmid DNA were irradiated at 277K with 238Pu alpha-particles or USX in the presence of 10(-4) to 0.33 mol dm(-3) Tris and the yields of SSB and DSB determined by gel electrophoresis. Computer simulations, using Monte Carlo track-structure codes for 1.5keV electrons (CPA100) and 3.2MeV alpha-particle track segments (PITS), were used to obtain yields of DNA SSB and DSB at different *OH scavenger conditions. RESULTS: The experimental yield of SSB and DSB induced by AlK USX and SSB induced by alpha-particles and the dependences on the mean diffusion distance of the *OH are in reasonable agreement with the corresponding simulated yields and their corresponding dependences. However, for DSB induced by alpha-particles, a significant systematic difference exists between the simulated and experimental yields over the full *OH scavenging range, with the simulated yields being a factor of two to three greater than the experimental values. CONCLUSION: That the simulated yields of strand breaks are generally in reasonable agreement with those determined experimentally over a wide range of *OH scavenging capacities, increases confidence in the use of these simulations as a valuable source of quantitative, mechanistic information on DNA damage induced at very low radiation doses.
Alpha Particles↗
High and low fluences of alpha-particles induce a G1 checkpoint in human diploid fibroblasts.
The effects of exposure to high and very low fluence alpha-particles on the G1 checkpoint were investigated in human diploid fibroblasts irradiated and released from density-inhibited confluent cultures by the use of the cumulative labeling index method. Transient and permanent arrests in G1 occurred in fibroblast populations exposed to mean doses as low as 1 cGy, suggesting that nontraversed bystander cells may contribute to the low dose response. In cells exposed to high fluences, the G1 checkpoint is at least as extensive as in gamma-irradiated cells. In contrast to gamma-irradiated cells, neither repair of potentially lethal damage nor a reduction in the fraction of cells transiently or permanently arrested in G1 were observed in cells held in confluence for 6 h after alpha-particle irradiation. Studies with isogenic wild-type, p53-/-, and p21Waf1-/- mouse embryo fibroblasts exposed to either gamma or alpha-particle radiation revealed a total lack of G1 arrest in either p53-/- or p21waf1-/- cells, indicating that the G1 checkpoint in wild-type cells is p53-dependent and that p21Wf1 fully mediates the role of p53 in its induction. In contrast to human cells, mouse embryo fibroblasts do not undergo a permanent G1 arrest. Except under conditions favoring potentially lethal damage repair, a comparable expression pattern of p53, p21Waf1, and other cell cycle-regulated proteins (pRb, p34cdc2, and cyclin B1) was observed in alpha-particle or gamma-irradiated human fibroblasts.
Alpha Particles↗
An alpha-particle emitting antibody ([213Bi]J591) for radioimmunotherapy of prostate cancer.
A novel alpha-particle emitting monoclonal antibody construct targeting the external domain of prostate-specific membrane antigen (PSMA) was prepared and evaluated in vitro and in vivo. The chelating agent, N-[2-amino-3-(p-isothiocyanatophen-yl)propyl]-trans-cyclohexane-1, 2-diamine-N,N',N',N'',N''-pentaacetic acid, was appended to J591 monoclonal antibody to stably bind the 213Bi radiometal ion. Bismuth-213 is a short-lived (t 1/2 = 46 min) radionuclide that emits high energy alpha-particles with an effective range of 0.07-0.10 mm that are ideally suited to treating single-celled neoplasms and micrometastatic carcinomas. The LNCaP prostate cancer cell line had an estimated 180,000 molecules of PSMA per cell; J591 bound to PSMA with a 3-nM affinity. After binding, the radiolabeled construct-antigen complex was rapidly internalized into the cell, carrying the radiometal inside. [213Bi]J591 was specifically cytotoxic to LNCaP. The LD50 value of [213Bi]J591 was 220 nCi/ml at a specific activity of 6.4 Ci/g. The potency and specificity of [213Bi]J591 directed against LNCaP spheroids, an in vitro model for micrometastatic cancer, also was investigated. [213Bi]J591 effectively stopped growth of LNCaP spheroids relative to an equivalent dose of the irrelevant control [213Bi]HuM195 or unlabeled J591. Cytotoxicity experiments in vivo were carried out in an athymic nude mouse model with an i.m. xenograft of LNCaP cells. [213Bi]J591 was able to significantly improve (P < 0.0031) median tumor-free survival (54 days) in these experiments relative to treatment with irrelevant control [213Bi]HuM195 (33 days), or no treatment (31 days). Prostate-specific antigen (PSA) was also specifically reduced in treated animals. At day 51, mean PSA values were 104 ng/ml +/- 54 ng/ml (n = 4, untreated animals), 66 ng/ml +/- 16 ng/ml (n = 6, animals treated with [213Bi]HuM195), and 28 ng/ml +/- 22 ng/ml (n = 6, animals treated with [213Bi]J591). The reduction of PSA levels in mice treated with [213Bi]J591 relative to mice treated with [213Bi]HuM195 and untreated control animals was significant with P < 0.007 and P < 0.0136, respectively. In conclusion, a novel [213Bi]-radiolabeled J591 has been constructed that selectively delivers alpha-particles to prostate cancer cells for potent and specific killing in vitro and in vivo.
Alpha Particles↗
Alpha particle radio-immunotherapy: animal models and clinical prospects.
Short-lived isotopes that emit alpha particles have a number of physical characteristics which make them attractive candidates for radioimmunotherapy. Among these characteristics are high linear energy transfer and correspondingly high cytotoxicity; particle range limited to several cell diameters from the parent atom; low potential for repair of alpha-induced DNA damage; and low dependence on dose rate and oxygen enhancement effects. This report reviews the synthesis, testing and use in animal models of an alpha particle emitting radioimmunoconjugate constructed via the noncovalent chelation of Bismuth-212 to a monoclonal IgM antibody specific for the murine T cells/neuroectodermal surface antigen, Thy 1.2. These 212Bi-anti-Thy 1.2 immunoconjugates are capable of extraordinary cytotoxicity in vitro, requiring approximately three 212Bi-labeled conjugates per target cell to suppress 3H-thymidine incorporation to background levels. The antigen specificity afforded by the monoclonal antibody contributes a factor of approximately 40 to the radiotoxicity of the immunoconjugate. Animals inoculated with a Thy 1.2+ malignant ascites were cured of their tumor in an antigen-specific fashion by intraperitoneal doses of approximately 200 microCi per mouse. Alpha particle emitting radioimmunoconjugates show great potential for regional and intracavitary molecular radiotherapy.
Alpha Particles↗
The biological effectiveness of radon-progeny alpha particles. IV. Morphological transformation of Syrian hamster embryo cells at low doses.
Primary explants of Syrian hamster embryo (SHE) cells were exposed to either low-LET 250 kVp X rays or graded single doses of defined high-LET alpha particles (90, 100, 120, 150, 180 and 200 keV/microns), simulating those produced by radon progeny, and monitored for cell inactivation and oncogenic transformation. For the alpha particles the doses delivered ranged from 1 cGy to 1 Gy with an emphasis on doses less than 20 cGy, while for the X rays the doses ranged from 20 cGy to 4 Gy. The dose-response curves for cell killing by alpha particles approximated an exponential function of dose, whereas the X rays produced a curve with a shoulder characteristic of linear-quadratic relationships seen for low-LET radiations. The RBE at 10% survival varied between 3.6-7.0 depending on the LET of the alpha particles, with the RBEm ranging between 7-12. The most effective alpha particles were those with an LET of 120 keV/microns. All radiations produced initial increases in the frequency of morphological transformants, as a function of dose, with a rise to a maximum followed by a plateau in the response which was relatively constant at approximately 2-6 x 10(-3) transformants frequency, expressed per initial cell at risk, had a tendency to decline to parallel the cell survival response. Both the dose at which the maximum frequency of transformants was expressed and the initial slope of the dose-response relationship differed substantially between the different radiation qualities. Maximal transformation per initial cell at risk occurred at doses as low as 1-4 cGy for the 90 and 100 keV/microns particles with the maximum occurring at higher doses (to 16 cGy) as the LET increased toward 200 keV/microns. In contrast, the maximal transformation for 250 kVp X rays was at 50 cGy. The 90 and 100 keV/microns particles, with an RBEm of 60 and 37, respectively, based on the ratios of the initial slopes of the dose-response curves, were the most effective LETs in terms of the ability to induce morphological transformation of SHE cells. When expressed in terms of particle fluence, it appears that in the LET range of radon progeny approximately two to four particle traversals per nucleus are required per killing event, whereas it is at doses corresponding to less than one particle per nucleus that maximal oncogenic transformation is expressed.(ABSTRACT TRUNCATED AT 400 WORDS)
Alpha Particles↗
Morphological, biochemical, and molecular changes in endothelial cells after alpha-particle irradiation.
The response of cultured bovine aortic endothelial (BAE) cells after exposure to alpha-particle radiation from chelated 212Bi has been evaluated. The results suggest that even relatively high doses of alpha-particle radiation from 212Bi (20-72 Gy) cause only minor acute changes in the morphology of BAE cells (light and electron microscopy) under conditions of confluent monolayer growth. Significant morphological changes can be detected in cells that detach from the monolayer, though it is unclear whether these changes represent a genuine response to irradiation or reflect the causes or effects of monolayer detachment with the consequent loss of intercellular biochemical communication. After alpha-particle irradiation (20-40 Gy) angiotensin-converting-enzyme activity was not detectable in the monolayer culture medium but was significantly decreased within the cell monolayer. Neutral-elution-assay data demonstrated that DNA double-strand-break (DSB) damage occurred in these cells and that about 35% of the DSBs were repairable.
Alpha Particles↗
An experimental analysis of some of the factors affecting gross alpha-particle activity with an emphasis on 226Ra and its progeny.
This work presents an experimental investigation of the measurement of the gross alpha-particle activity of water samples by EPA Method 900.0. The residue produced in Method 900.0 is modeled by a BaSO4 precipitate distributed over a planchet. The dependence of the gross alpha-particle activity on the activity of Ra and its progeny, on the residue mass and geometry, and on the time between sample preparation and analysis is studied. It is shown that these factors can cause the gross alpha-particle activity of a sample to vary by more than a factor of three for replicate samples and to significantly overestimate the alpha activity of the residue. For a given sample geometry, the gross-alpha particle activity generally increases as the residue mass increases owing to the presence of the radium progeny.
Alpha Particles↗
The effect of dimethyl sulfoxide on the induction of DNA double-strand breaks in V79-4 mammalian cells by alpha particles.
The present study was undertaken to assess the protective effect of dimethyl sulfoxide (DMSO) against the induction and rejoining of DNA double-strand breaks (DSBs) and inactivation of V79-4 Chinese hamster cells by both high- and low-linear energy transfer (LET) radiations. The cells were exposed under aerobic conditions as monolayers to either low-LET photons (60Co gamma rays) or high-LET alpha particles (238Pu) at 277 K. The initial yield of DSBs, determined by elution under nondenaturing conditions, is linearly dependent on dose. When the irradiation was carried out in the presence of DMSO (0-0.6 mol dm-3), the initial yields of DSBs induced by both gamma and alpha-particle irradiation decrease. With gamma irradiation at [DMSO] > 0.6 mol dm-3, a further decrease in the yield of DSBs occurs. DMSO (0.5 mol dm-3) reduces the initial yield of DSBs by 50 +/- 5% and 32 +/- 4% for photons and alpha particles, respectively. DMSO protects more effectively against cellular inactivation and DSB induction at low LET compared with alpha-particle irradiation with protection factors of 1.7 and 1.4, respectively, for survival and 2.0 and 1.5, respectively, for DSBs. After incubation of the irradiated cells for 3 h at 310 K after high-LET irradiation, the residual yield of DSBs is reduced by < 13% when the irradiations were carried out in the presence of 0.5 mol dm-3 DMSO. With gamma irradiation in the presence of 0.5 mol dm-3 DMSO, 90% of the DSBs are rejoined by 3 h incubation at 310 K. Therefore, the nonscavengeable DSBs induced by alpha particles are not significantly rejoined within 3 h, in contrast to rejoining of the majority of the nonscavengeable DSBs induced by gamma irradiation. From comparison of the data on DSBs and survival for alpha-particle irradiation, it is inferred that the severity of damage is reduced by DMSO through minimizing the formation of OH-induced sugar/base modifications in the vicinity of nonscavengeable DSBs.
Alpha Particles↗
A multi-port low-fluence alpha-particle irradiator: fabrication, testing and benchmark radiobiological studies.
A new multi-port irradiator, designed to facilitate the study of the effects of low fluences of alpha particles on monolayer cultures, has been developed. The irradiator consists of four individual planar (241)Am alpha-particle sources that are housed inside a helium-filled Lucite chamber. Three of the radioactive sources consist of 20 MBq of (241)Am dioxide foil. The fourth source, used to produce higher dose rates, has an activity of 500 MBq. The four sources are mounted on rotating turntables parallel to their respective 1.5-microm-thick Mylar exit windows. A stainless steel honeycomb collimator is placed between the four sources and their exit windows by a cantilever attachment to the platform of an orbital shaker that moves its table in an orbit of 2 cm. Each exit window is equipped with a beam delimiter to optimize the uniformity of the beam and with a high-precision electronic shutter. Opening and closing of the shutters is controlled with a high-precision timer. Custom-designed stainless steel Mylar-bottomed culture dishes are placed on an adapter on the shutter. The alpha particles that strike the cells have a mean energy of 2.9 MeV. The corresponding LET distribution of the particles has a mean value of 132 keV/microm. Clonogenic cell survival experiments with AG1522 human fibroblasts indicate that the RBE of the alpha particles compared to (137)Cs gamma rays is about 7.6 for this biological end point.
Alpha Particles↗
Design, spectrum measurements and simulations for a 238Pu alpha-particle irradiator for bystander effect and genomic instability experiments.
Design, spectrum measurements and simulations for an alpha-particle irradiator for bystander effect and genomic instability experiments are presented. Measured alpha-particle energy spectra were used to confirm the characteristics of the source of the irradiator specified by the manufacturer of the source. The spectra were measured in vacuum with a high-resolution spectrometer and simulated with an AASI Monte Carlo code. As a next step, we simulated alpha-particle energy spectra at the target plane of the irradiator for three different source-to-target distances. In these simulations, helium was used as the medium between the source and the exit window of the irradiator; its pressure and temperature corresponded to those of the ambient air. Mean energies and full-widths at half-maximum (FWHM) were calculated for the three different helium gas tracks.
Alpha Particles↗
WAF1 accumulation by carbon-ion beam and alpha-particle irradiation in human glioblastoma cultured cells.
PURPOSE: There have been no reports about the effects of heavy-ion beams on the expression of the WAF1 gene, although ionizing radiation such as y-rays and X-rays is well known to induce WAF1 (p21/CIP1/sdi1) gene expression in a p53-dependent manner. In the present study, it was examined whether WAF1 accumulation was induced after carbon-ion (C-) beam or alpha-particle irradiation in four glioblastoma cell lines. MATERIALS AND METHODS: A colony assay for radiosensitivity and Western blot analysis of WAF1 were applied to two human glioblastoma cell lines, A-172 bearing wild-type p53 (wtp53) and T98G bearing mutated p53 (mp53). A-172/neo and A-172/mp53 were transfected with a control vector (containing only a neo selection marker) and a mp53 expression vector respectively. RESULTS: The amount of WAF1 increased markedly after X-ray irradiation in A-172 and A-172/neo cells but not in T98G and A-172/mp53 cells. The level of WAF1 reached a plateau at 3-10 h after X-ray irradiation at 5 Gy in A-172 and A-172/neo cells. Likewise, the levels of WAF1 in A-172 and A-172/neo cells reached a plateau at 3-10 h and 6-24 h after C-beam (3.0 Gy) and alpha-particle (4.5 Gy) irradiation respectively. The amount of WAF1 increased markedly in a dose-dependent manner 10 h after X-ray, C-beam or alpha-particle irradiation in A-172 and A-172/neo cells but not in T98G or A-172/mp53 cells. In addition, cell survival assay showed that these cell lines were most sensitive to C-beams, less sensitive to alpha-particles and least sensitive to X-rays at 10% survival. There was no difference in sensitivity among these cell lines against C-beam and alpha-particle irradiation whereas wtp53 cells (A-172 and A-172/neo) were more sensitive to X-rays than mp53 cells (A-172/mp53 and T98G). CONCLUSIONS: These results indicate that C-beams and alpha-particles induce p53-dependent WAF1 accumulation as well as is the case with X-rays, suggesting that WAF1 protein accumulation may not contribute to cell killing.
Alpha Particles↗
High-resolution alpha spectrometry under field conditions - fast identification of alpha particle emitting radionuclides from air samples.
Alpha particle emitting radionuclides may be released into the atmosphere as a result of a severe nuclear accident, the malevolent use of radioactive material or some other incident. Rapid detection methods are then of crucial importance for carrying out well-timed protective actions. The present paper demonstrates that a method in which an aerosol sample is collected on a filter and directly analysed by high-resolution alpha spectrometry in a vacuum chamber, but without radiochemical sample treatment, is suitable for field measurements. A detection limit of less than 0.1 Bqm(-3) for (239)Pu is achieved assuming 1-h sampling using a glass-fibre filter and 1-h data acquisition. This value is higher than in the case when sampling is performed using a porous membrane filter. A measurement system consisting of standard components is mounted in a vehicle designed for rapid field measurements.
Air Pollutants, Radioactive↗
The mutagenicity of alpha particles in Ehrlich ascites tumor cells.
Cell killing and the induction of mutation to thioguanine resistance (HGPRT enzyme deficiency) were measured after exposure of Ehrlich ascites tumor cells to 150-kV X rays and 241Am alpha particles. The curve describing the induction of mutations was almost linear after exposure to alpha particles (slope: 14.1 x 10(-5) Gy-1) but upward bending after exposure to X rays, apparently reaching a final slope to that obtained after exposure to alpha particles. The number of mutants induced per viable cell by alpha particles at a given level of cell killing was similar to that induced by X rays. The RBE values obtained for cell killing and the induction of mutations are compared with each other, and the possible involvement of repair processes in determining the RBE is discussed.
Alpha Particles↗
Cell detection in phase-contrast images used for alpha-particle track-etch dosimetry: a semi-automated approach.
A novel alpha-particle irradiator has recently been developed that provides the ability to characterize cell response. The irradiator is comprised of a collimated, planar alpha-particle source which, from below, irradiates cells cultured on a track-etch material. Cells are imaged using phase-contrast microscopy before and following irradiation to obtain geometric information and survival rates; these can be used with data from alpha-particle track images to assess cell response. A key step in this process is determining cell location within the pre-irradiation images. Although this can be done completely by a human observer, the number of images requiring analysis makes the process time-consuming and tedious. To reduce the potential human error and decrease user interaction time, a semi-automated, computer-aided method of cell detection has been developed. The method employs a two-level adaptive thresholding technique to obtain size and position information about potential cell cytoplasms and nuclei. Proximity and geometry-based thresholds are then used to mark structures as cells. False-positive detections from the automated algorithm are due mostly to imperfections in the track-etch background, camera effects and cellular residue. To correct for these, a human observer reviews all detected structures, discarding false positives. When analysing two randomly selected cell dish image databases, the semi-automated method detected 92-94% of all cells and 94-97% of cells with a well-defined cytoplasm and nucleus while reducing human workload by 32-83%.
Algorithms↗
Radiopharmaceutical chemistry of targeted radiotherapeutics, part 1: effects of solvent on the degradation of radiohalogenation precursors by 211At alpha-particles.
UNLABELLED: The high energy and short range of alpha-particles make them attractive for targeted radiotherapy. However, these properties can be problematic when the production of high activity levels of alpha-particle-emitting radiotherapeutics is required. For example, difficulties were encountered in the production of N-succinimidyl 3-[211At]-astatobenzoate (SAB), when 370-MBq doses of 211At-labeled antibody were required. The purpose of this study was to investigate a potential cause of this behavior--radiolytic degradation of the radiohalogenation precursor. METHODS: Both N-succinimidyl 3-(tri-n-butylstannyl)benzoate (BuSTB) and N-succinimidyl 3-trimethylstannylbenzoate (MeSTB) were incubated with various 211At time-activity combinations such that the radiation dose received by the reaction medium ranged from about 0 to 20,000 Gy. Studies were performed using chloroform, methanol, and benzene as the solvent, and both at neutral pH and at a pH of approximately 5.5, as used in SAB synthesis. The fraction of tin precursor remaining and the generation of unlabeled byproducts were determined from high-performance liquid chromatograms and then plotted against radiation dose. RESULTS: Extensive radiolytic decomposition of BuSTB and MeSTB was observed in chloroform, with 50% degradation taking place even at doses below 500 Gy. Formation of a byproduct, most likely N-succinimidyl 3-chlorobenzoate, increased with radiation dose. A greater degree of stability was seen in both methanol and benzene, with more than 85% of the precursor remaining at 3,500 Gy. No cold byproducts were observed with either solvent. CONCLUSION: The nature of the solvent profoundly influences the ability to synthesize high activity levels of SAB and possibly other 211At-labeled radiopharmaceuticals.
Alpha Particles↗
Alpha-particle-induced increases in the radioresistance of normal human bystander cells.
Numerous investigators have reported that direct exposure of cells to a low dose of ionizing radiation can induce a condition of enhanced radioresistance, i.e. a "radioadaptive" response. In this report, we investigated the hypothesis that a radioadaptive bystander effect may be induced in unirradiated cells by a transmissible factor(s) present in the supernatants of cells exposed to a low dose of alpha particles. Normal human lung fibroblasts (HFL-1) were irradiated with 1 cGy of alpha particles and their supernatants were transferred to unirradiated HFL-1 cells as a bystander cell model. Compared to directly irradiated cells that were not treated with supernatants from HFL-1 cells exposed to low-dose radiation, such treatment resulted in increased clonogenic survival after subsequent exposure to 10 and 19 cGy of alpha particles. Increases in protein levels of AP-endonuclease, a redox and DNA base excision repair protein, were found in the bystander cells, but not in directly irradiated cells. Supernatants from alpha-particle-irradiated cells were also found to increase the clonogenicity of unirradiated cells. These results, in conjunction with our earlier findings that supernatants from cells exposed to a low dose of alpha particles contain growth-promoting activity, suggest that this new bystander effect may be related to an increase in DNA repair and cell growth/cell cycle regulation.
Adaptation, Physiological↗
Distributions of cell populations within alpha-particle range of plutonium deposits in the rat and beagle testis.
Plutonium is not uniformly distributed in testicular tissues; thus some cell populations may receive larger or smaller radiation exposures than would be expected if the nuclide were uniformly distributed. The distributions of cell populations within alpha-particle range of Pu deposits in rat and beagle testes were determined. The data were collected from autoradiographs of testicular tissues containing 241Pu. A cell distribution factor (CDF) was determined for each cell population and is defined as the average number of each cell type within alpha-particle range of each observed Pu deposit relative to the number of each cell type that would be expected within alpha-particle range of each Pu deposit, if the deposits were distributed uniformly. In addition, the percentage of the spermatogonial stem cell population within alpha-particle range of Pu deposits was determined. In rats, the CDF for the spermatogonial stem cells is about 2.2. This value is similar to other enhancement and inhomogeneity factors reported for rodents in the literature. In beagles the CDFs to all cells in the seminiferous epithelium were less than the rats. In addition, the percentage of spermatogonial cells within alpha-particle range of Pu concentrations in the interstitial tissues was a factor of about 3 less in the dog than in the rat. The largest CDFs seen in both species were in the interstitial tissues, particularly for Leydig cells. Because the organization of testicular tissues in the beagle is quite different from rodents but more similar to human, the results from this study suggest that extrapolations from rodents to humans may tend to overestimate the potential for radiation exposure to spermatogonial stem cells as well as the fraction of the spermatogonial stem cell population at risk to exposure from internally deposited 239Pu.
Alpha Particles↗