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Molecular analysis and comparison of radiation-induced large deletions of the HPRT locus in primary human skin fibroblasts.

Genetic alterations in gamma-ray- and alpha-particle-induced HPRT mutants were examined by multiplex polymerase chain reaction (PCR) analysis. A total of 39-63% of gamma-ray-induced and 31-57% of alpha-particle-induced mutants had partial or total deletions of the HPRT gene. The proportion of these deletion events was dependent on radiation dose, and at the resolution limits employed there were no significant differences between the spectra induced by equitoxic doses of alpha particles (0.2-0.4 Gy) and gamma rays (3 Gy). The molecular nature of the deletions was analyzed by the use of sequence tagged site (STS) primers and PCR amplification as a "probe" for specific regions of the human X chromosome within the Xq26 region. These STSs were closely linked and spanned regions approximately 1.7 Mbp from the telomeric side and 1.7 Mbp from the centromeric side of the HPRT gene. These markers include: DXS53, 299R, DXS79, yH3L, 3/19, PR1, PR25, H2, yH3R, 1/44, 1/67, 1/1, DXS86, D8C6, DXS10 and DXS144. STS analyses indicated that the maximum size of total deletions in radiation-induced HPRT mutants can be greater than 2.7 Mbp and deletion size appears to be dependent on radiation dose. There were no apparent differences in the sizes of the deletions induced by alpha particles or gamma rays. On the other hand, deletions containing portions of the HPRT gene were observed to be 800 kbp or less, and the pattern of the partial deletion induced by alpha particles appeared to be different from that induced by gamma rays.

Alpha Particles↗

The signal recognition particle receptor alpha subunit assembles co-translationally on the endoplasmic reticulum membrane during an mRNA-encoded translation pause in vitro.

Many proteins, including the alpha subunit of the signal recognition particle receptor (SR alpha), are targeted within the cell by poorly defined mechanisms. A 140 residue N-terminal domain of SR alpha targets and anchors the polypeptide to the endoplasmic reticulum membrane by a mechanism independent of the pathway involving the signal recognition particle. To investigate the mechanism of membrane anchoring, translation pause sites on the SR alpha mRNA were used to examine the targeting of translation intermediates. A strong pause site at nucleotide 507 of the mRNA open reading frame corresponded with the shortest nascent SR alpha polypeptide able to assemble on membranes. An mRNA sequence at this pause site that resembles a class of viral -1 frameshift sequences caused translation pausing when transferred into another mRNA context. Site-directed mutagenesis of the mRNA greatly reduced translation pausing without altering the polypeptide sequence, demonstrating unambiguously a role for this mRNA sequence in translation pausing. SR alpha polypeptides synthesized from the non-pausing mRNA were impaired in co-translational membrane anchoring. Furthermore, co-translational membrane assembly of SR alpha appears to anchor polysomes translating SR alpha to membranes.

Animals↗

Synthetic diamonds as ionisation chamber radiation detectors in biological environments.

Synthetic diamonds with nitrogen concentrations higher than previously reported in the literature are found to operate very effectively as alpha-particle detectors, as well as detectors for gamma radiation, when operated as ionisation chambers. Certain of the specimens exhibited extensive linear response characteristics when subjected to either alpha particles or gamma radiation of various dose rates. For alpha particles, the response of the detectors at constant particle flux was also found to increase linearly with increasing alpha-particle energy. Unlike previously reported investigations, however, the variation in the response of the synthetic stones to gamma radiation as a function of time was found to be not only more rapid but also to be virtually unaffected by illumination with intense white light.

Alpha Particles↗

Radiation effect on positronium formation in solid state nuclear track detector.

The effect of alpha-particles on CR-39, a material used in solid state nuclear track detectors (SSNTDs), has been investigated using the positron annihilation lifetime (PAL) technique. The samples were irradiated using a (238)Pu alpha-source of energy ranging from 1 to 5 MeV and with different doses ranging from 0 to 57.87 mGy. The ortho-positronium (o-Ps) lifetime, tau(3), shows a slight increase as the irradiation dose increases, while a rapid change in the o-Ps intensity, I(3) at 10 mGy was found. In addition, the PAL parameters (tau(3), I(3)) have been studied as a function of the energy of alpha-particles. The obtained results indicate that the o-Ps lifetime increases slightly with increasing energy of the alpha-particle. On the other hand, the o-Ps intensity decreases exponentially with increasing alpha-particle energy, plateaus, and finally increases. The data show that the track diameter increases with decreasing energy of the alpha-particle, while the track density increases with increasing the irradiation dose. A correlation between the track diameter and the o-Ps hole diameter was observed.

Journal Article↗

Radon, tobacco-specific nitrosamine and mutagenesis in mammalian cells.

The mutagenicity of 4-methylnitrosamine-1-3-pyridyl-1-butanone (NNK), either alone or in combination with low dose alpha particle irradiation, was examined using the human-hamster hybrid (A(L)) cell assay. NNK induced a dose-dependent toxicity in A(L) cells. In combination with a 25 cGy dose of alpha particles, the induced survival fraction fell within the statistical range of the calculated values assuming an additive interaction of the two agents. In addition, NNK is mutagenic in A(L) cells at the CD59 locus. Furthermore, a low dose of NNK, when combined with radon alpha particles, resulted in a combined mutagenic effect in A(L) cells that was consistent with an additive model but less than additive at higher NNK concentrations. The majority of NNK induced CD59(-) mutants (77.6%) lost at least one additional marker in addition to the CD59 which encodes the cell surface antigen. When combined with alpha particles, the proportion of mutants with additional marker loss increased with increasing dose of NNK. Our study further confirms that NNK is mutagenic in mammalian cells, induces mostly deletions, and provides an in vitro assessment of the combined genotoxic effects of NNK and alpha particles at low environmentally relevant doses. This finding should be helpful in understanding the molecular mechanism of the mutagenic process as a result of multi-agent interaction.

Alpha Particles↗

Large angle elastic alpha scattering on a N=Z nucleus above A=40.

Scattering of alpha particles from 44Ti, the lightest unstable alpha-particle nucleus above A=40, has been measured at backward angles. The "anomalous" order-of-magnitude enhancement that is characteristic of 40Ca and other light alpha-particle nuclei is not observed. Instead, the backward yield is similar to that observed for other nuclei heavier than 40Ca, and is well described with average optical model parameters.

Journal Article↗

Mechanism of the Shape and Structure Control of Monodispersed alpha-Fe2O3 Particles by Sulfate Ions.

The characteristics of the adsorption of sulfate ions to hematite (alpha-Fe2O3) particles have been studied to elucidate the anisotropic growth of hematite particles in the presence of sulfate ions. Sulfate ions were actually found to be most strongly adsorbed to crystal faces parallel to the c-axis of the hexagonal crystal system from the adsorption isotherms of sulfate to hematite particles of different crystal habits, in accord with the retardation of their growth in the direction normal to the c-axis. It was found from FTIR spectroscopy that the adsorbed sulfate ions on the faces parallel to the c-axis, such as the {110} and {100} faces, or on {012} faces took the bidentate structure to Fe ions on the surfaces, while a monodentate structure was suggested for sulfate ions on the c-planes ({001} faces). The adsorbed amount of sulfate ions to the {012} faces of hematite at 100 degreesC decreased with increasing pH and became almost zero at pH >/=5, suggesting that the shape control with sulfate is possible only in the acidic media at pH < 5. EDX and chemical analysis revealed that sulfate ions were almost uniformly incorporated into the ellipsoidal or peanut-type particles during their growth in the presence of sulfate ions. On the other hand, sulfate ions in the solution phase with a high concentration of chloride ions such as 3.0 mol dm-3 were likely to be present in the form of free ions without forming a complex with Fe3+, as suggested from UV spectroscopy at 25 degreesC. When the concentration of sulfate ions in the solution phase exceeded the level for shape control of hematite, precipitation of acicular alpha-FeOOH (goethite) was observed. If hematite particles were present in such a system, alpha-FeOOH was grown as whiskers on the hematite particles. When [SO2-4] in the solution phase was higher than 0.1 mol dm-3, precipitation of basic ferric sulfate was also observed in addition to the growth of alpha-FeOOH whiskers on hematite. Copyright 1998 Academic Press.

Journal Article↗

Absolute humidity measurement utilizing alpha-ray absorption.

Changes in air density due to humidity were measured by a scintillation detector with alpha-particles. The distance between the scintillator and an alpha-ray source of 241 Am, 3.7 MBq (100 microCi), was fixed at 25 mm which was a little shorter than the range of alpha-particles from the source. The measured absolute humidities were in a range of 7.9 g/m3 to 52.2 g/m3 at temperatures of 35 degrees C and 45 degrees C and under atmospheric pressure. The counting rate of alpha-particles in an absolute humidity of 31.7 g/m3 (80% in relative humidity) at 35 degrees C increased 28% compared with that in dry air. From experimental results and theoretical calculation, the counting rate difference between humid air and dry air was shown to be almost proportional to the absolute humidity in air. The absolute humidity can be measured with an accuracy of +/- 3 g/m3, that is +/- 5% in relative humidity at 45 degrees C.

Alpha Particles↗

Inhibition of ribosomal RNA synthesis in yeast by ionizing radiations.

The effects of ionizing radiations on transcriptional activity were studied in the diploid yeast Saccharomyces cerevisiae. As experimental indicator the synthesis of ribosomal RNA (r-RNA) was measured for 1 h after exposure of cells to gamma-rays, X-rays or alpha-particles. gamma- or X-ray induced transcription inhibition was always found to decrease exponentially with dose. D0 values of 2150 or 1950 Gy were determined in wild-type cells, corresponding to a mean energy of about 60 eV per r-RNA gene. The finding of differential sensitivities of the two high molecular-weight r-RNA species which are cotranscribed from r-DNA is compatible with the existence of a transcription terminating mechanism. Cells from a mutant strain (rad-9), radiation sensitive with respect to colony forming ability, show an approximately equal sensitivity for transcription inhibition compared to the wild-type (D0 (2095) = 2400 Gy). Inactivation of r-RNA synthesis in cells exposed to alpha-particles at room-temperature showed a decreased sensitivity with higher particle fluences ('resistant tail'). This phenomenon, however, was drastically reduced if the temperature during irradiation was lowered to 4 degrees C, and was completely abolished when dried cells were used. The results may be explained by the presence of recovery processes in vegetative cells during prolonged exposures to alpha-particles at room temperature. An inactivation cross-section for alpha-particle induced transcription inhibition of about 0.02 micron 2 can be derived from the experimental data. When comparing this value with the estimated target volume, it appears that no single genes but the whole cluster of about 120 r-RNA genes on each of the chromosomes XII in the diploid cell may be inactivated by a single alpha-particle.

Alpha Particles↗

Long-range alpha detector.

Historically, alpha-particle detectors have been limited by the very short range of alpha particles in air. This results in a number of problems inherent to alpha contamination detectors, such as relatively poor sensitivity, geometry limitations, and inefficient monitoring techniques. In this paper, we document tests of a new long-range alpha detector. The charges generated by the interaction of alpha particles with air can be transported over significant distances (several meters) in a moving current of air generated by a small fan. An ion chamber located in front of the fan measures the current carried by the moving ions and, hence, detects the alpha decays.

Alpha Particles↗

The influence of radiation quality on radiation-induced hemolysis and hemoglobin oxidation of human erythrocytes.

Human erythrocytes were exposed to gamma-rays and alpha-particles to assess radiation-induced membrane damage and hemoglobin oxidation and denaturation. With all parameters measured, the alpha-particles proved to be less efficient than the gamma-rays. The time-dependence of hemolysis showed also clear differences: with the gamma-rays the process was faster, reaching saturation after 40-90 min (depending on dose), but with the alpha-particles the final level was attained only after about 3-7 h. Hemoglobin oxidation and denaturation could be measured only after gamma-exposure, but they were negligible with the alpha-particles when comparable doses were applied. These results are interpreted by proposing that OH-radicals, whose yields are smaller with densely ionizing radiation, play a crucial role in the induction of the processes for radiation-induced erythrocyte damage.

Alpha Particles↗

Kinetics of chromosome rejoining in normal human fibroblasts after exposure to low- and high-LET radiations.

To determine whether chromosome breaks produced by alpha particles are processed differently from those produced by X rays, the premature chromosome condensation technique was used to follow chromosome rejoining after irradiation. Doses of 90 and 200 keV/microns alpha particles (2.7 Gy) and 250 kVp X rays (6 Gy) were chosen to produce approximately the same number of initial chromosome breaks (about 30 excess fragments per cell). Frequencies of excess fragments were assessed at eight times to 24 h after irradiation with the final yields being about 2, 4 and 8 excess fragments per cell for 250 kVp X rays and 200 and 90 keV/microns alpha particles, respectively. For each radiation the time for the initial measured fragment frequency per cell to be halved (i.e. to about 15) was the same (about 100 min). The results were fitted to three models of kinetics of the rejoining, and the initial and residual number of excess chromosome fragments as well as the rate of rejoining were determined. Even with eight times, discrimination between the models of the kinetics was not possible, such that a single-component first-order reaction could not be rejected for either X-ray- or alpha-particle-induced breaks. Although rejoining proceeds at similar rates, the probability of "correct" rejoining is apparently reduced for alpha-particle-irradiated cells.

Chromosomes↗

SOURCES: a code for calculating (alpha,n), spontaneous fission, and delayed neutron sources and spectra.

SOURCES is a computer code that determines neutron production rates and spectra from (alpha,n) reactions, spontaneous fission and delayed neutron emission owing to the decay of radionuclides in homogeneous media, interface problems and three-region interface problems. The code is also capable of calculating the neutron production rates due to (alpha,n) reactions induced by a monoenergetic beam of alpha particles incident on a slab of target material. The (alpha,n) spectra are calculated using an assumed isotropic angular distribution in the centre-of-mass system with a library of 107 nuclide decay alpha-particle spectra, 24 sets of measured and/or evaluated (alpha,n) cross sections and product nuclide level branching fractions, and functional alpha particle stopping cross sections for Z < 106. Spontaneous fission sources and spectra are calculated with evaluated half-life, spontaneous fission branching and Watt spectrum parameters for 44 actinides. The delayed neutron spectra are taken from an evaluated library of 105 precursors. The code outputs the magnitude and spectra of the resultant neutron sources. It also provides an analysis of the contributions to that source by each nuclide in the problem.

Algorithms↗

Induction of DNA-protein crosslinks in Chinese hamster V79-4 cells exposed to high- and low-linear energy transfer radiation.

The induction of DNA-protein crosslinks (DPCs) in Chinese hamster V79-4 cells after irradiation under hypoxic and aerobic conditions at 277 K with 60Co gamma rays, 238Pu alpha particles and aluminum K (Al(K)) ultrasoft X rays has been determined using a nitrocellulose filter binding assay. The dose dependences for the induction of DPCs, which involves covalent linkage, are linear over the absorbed dose range used (0-400 Gy with alpha-particle and gamma radiation, 0-600 Gy with Al(K) X rays). The yield of DPCs induced under hypoxic conditions is 55, 51 and 25 DPCs per gray per cell for 60Co gamma rays, alpha particles and Al(K) X rays, respectively. The yield of DPCs is significantly reduced in the presence of oxygen by 20, 50 and 79% for 60Co gamma rays, alpha particles and Al(K) X rays, respectively. Since the mean size of the DNA attached to the protein is uniform for 60Co gamma rays and alpha particles, variations in the DNA size do not influence the yields of DPCs. Although a DPC may be considered as a complex lesion combining two macromolecules, the dependence of the yield of DPCs on LET does not reflect the ionizing density of the radiations used. Further, this dependence on LET and the effect of oxygen do not reflect the corresponding dependences determined for a variety of biological responses. From these findings and knowledge of the radiation tracks, it is proposed that DPCs induced particularly under aerobic conditions with 60Co gamma rays are formed mainly in the sparsely ionizing segments of the radiation track.

Animals↗

Some observations on the structure of Suncus liver with special reference to the vitamin A-storing cell.

The structure of the liver of the thick-tailed shrew (Suncus murinus) was studied with special reference to the vitamin A-storing cell. The macroscopic arrangement of hepatic lobes was the same as those of rodents. Connective tissues of Glisson's sheath were not prominent. There were gradual differences in the size and the cytoplasmic contents of hepatocytes among perihepatic, intermediate, and periportal regions. These correspond to the acinar zones 3, 2, and 1 of Rappaport, respectively. The ultrastructural features of the hepatocyte were numerous microvilli, a large mass of glycogen particles (alpha-particles), and well-developed Golgi complexes and lysosomes in the peribiliary region. Cellular elements of the sinusoid were the same as those of rodents. Vitamin A-storing cells were demonstrated by autoradiography of tritiated retinyl acetate administered orally. They were distributed in the perihepatic and intermediate regions. The number of vitamin A-storing cells was much smaller than that in the mouse liver and did not increase after excess vitamin A was given to the animal. Cytological features of the vitamin A-storing cells in Suncus liver were similar to those for other mammalian livers. The scarceness of vitamin A-storing cells and the low amount of vitamin A esters suggest that Suncus does not store much vitamin A in the liver.

Adipose Tissue↗

Evaluation of an internal cyclotron target for the production of 211At via the 209Bi (alpha,2n)211 at reaction.

Astatine-211 is a 7.2 h half-life alpha-emitting radionuclide which has shown great promise for targeted radiotherapy. It is generally produced by cyclotron bombardment of bismuth metal targets with 28 MeV alpha-particles via the 209Bi(alpha,2n)211 At reaction. In order to provide 211At activity levels anticipated for clinical investigations, an internal target system has been designed and evaluated. The system has a grazing-angle configuration and leading- and trailing-edge monitors. Both aluminum and copper target backings were evaluated. With approx. 28 MeV alpha-particles, the 211At production efficiency was 41 +/- 7 MBq/microA.h, compared with 10.6 +/- 1.2 MBq/microA.h for an external target. Radionuclidic purity of 211At was high with no evidence of 210At.

Astatine↗

Ordered synthesis and mobilization of glycogen in the perfused heart.

The molecular order of synthesis and mobilization of glycogen in the perfused heart was studied by 13C NMR. By varying the glucose isotopomer ([1-13C]glucose or [2-13C]glucose) supplied to the heart, glycogen synthesized at different times during the perfusion was labeled at different carbon sites. Subsequently, the in situ mobilization of glycogen during ischemia was observed by detection of labeled lactate derived from glycolysis of the glucosyl monomers. When [1-13C]glucose was given initially in the perfusion and [2-13C]glucose was given second, [2-13C]lactate was detected first during ischemia and [3-13C]lactate second. This result, and the equivalent result when the glucose labels were given in the reverse order, demonstrates that glycogen synthesis and mobilization are ordered in the heart, where glycogen is found morphologically only as beta particles. Previous studies of glycogen synthesis and mobilization in liver and adipocytes [Devos, P., & Hers, H.-G. (1979) Eur. J. Biochem. 99, 161-167; Devos, P., & Hers, H.-G. (1980) Biochem. Biophys. Res. Commun. 95, 1031-1036] have suggested that the organization of beta particles into alpha particles was partially responsible for ordered synthesis and mobilization. The observations reported here for cardiac glycogen suggest that another mechanism is responsible. In addition to examining the ordered synthesis and mobilization of cardiac glycogen, we have selectively monitored the NMR properties of 13C-labeled glycogen synthesized early in the perfusion during further glycogen synthesis from a second, differently labeled substrate. During synthesis from the second labeled glucose monomer, the glycogen resonance from the first label decreased in integrated intensity and increased in line width.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗

Calculation of the neutron W value for neutron dosimetry below the MeV energy region.

The effective neutron W value for tissue-equivalent gas in the energy region from 5 keV to 5.7 MeV has been calculated using W values for recoil particles (protons, alpha particles, oxygen, carbon and nitrogen ions), which are produced by incident neutrons. The W value is assumed to be an energy-fluence-average over the W values of the recoil particles. The energy fluence spectra for the recoil particles are calculated by using a continuous slowing down approximation (CSDA). For the W values of recoil particles in the low-energy region, the recently evaluated data by Siebert et al and Taylor et al were used. Results are presented which show that the effective neutron W value depends strongly on energy in the low-energy region. This result indicates that neutron dose measurements using ionization chambers need a considerable correction of the W value in the low-energy region.

Carbon↗