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1.
The functioning of radon diffusion chambers was studied using the Monte Carlo code RAMMX developed here. The alpha particles from radon are assumed randomly produced in the volume of the cylinder, and those from the progeny are assumed to originate randomly at the cylindrical surface. The energy spectrum, the distribution of incident angles, and the distribution of path lengths of the alpha particles on the detector were obtained. These quantities vary depending on input parameters such as initial alpha particle energy, radius and depth of the diffusion chamber, detector size and atmospheric pressure. The calculated energy spectrum for both 222Rn and 220Rn was compared with experiment, permitting the identification of each peak and its origin, and a better understanding of radon monitoring. Three aspects not considered in previous calculations are progeny alphas coming from surfaces of the monitor, taking into account the atmospheric pressure, and including the isotope 220Rn. 相似文献
2.
We report results of air monitoring started due to the recent natural catastrophe on 11 March 2011 in Japan and the severe ensuing damage to the Fukushima Dai-ichi nuclear reactor complex. On 17-18 March 2011, we registered the first arrival of the airborne fission products 131I, 132I, 132Te, 134Cs, and 137Cs in Seattle, WA, USA, by identifying their characteristic gamma rays using a germanium detector. We measured the evolution of the activities over a period of 23 days at the end of which the activities had mostly fallen below our detection limit. The highest detected activity from radionuclides attached to particulate matter amounted to 4.4 ± 1.3 mBq m −3 of 131I on 19-20 March. 相似文献
3.
The first nuclear explosion test, named the Trinity test, was conducted on July 16, 1945 near Alamogordo, New Mexico. In the tremendous heat of the explosion, the radioactive debris fused with the local soil into a glassy material named Trinitite. Selected Trinitite samples from ground zero (GZ) of the test site were investigated in detail for radioactivity. The techniques used included alpha spectrometry, high-efficiency gamma-ray spectrometry, and low-background beta counting, following the radiochemistry for selected radionuclides. Specific activities were determined for fission products (90Sr, 137Cs), activation products (60Co, 133Ba, 152Eu, 154Eu, 238Pu, 241Pu), and the remnants of the nuclear fuel (239Pu, 240Pu). Additionally, specific activities of three natural radionuclides (40K, 232Th, 238U) and their progeny were measured. The determined specific activities of radionuclides and their relationships are interpreted in the context of the fission process, chemical behavior of the elements, as well as the nuclear explosion phenomenology. 相似文献
4.
Cigarette smoking is one of the pathways that might contribute significantly to the increase in the radiation dose reaching man, due to the relatively large concentrations of 210Pb and 210Po found in tobacco leaves. In the present study, the concentrations of these two radionuclides were determined in eight of the most frequently sold cigarette brands produced in Brazil. 210Pb was determined by counting the beta activity of 210Bi with a gas flow proportional detector after radiochemical separation and precipitation of PbCrO4. 210Po was determined by alpha spectrometry using a surface barrier detector after radiochemical separation and spontaneous deposition of Po on a copper disk. The results showed concentrations ranging from 11.9 to 30.2 mBq per gram of dry tobacco for 210Pb and from 10.9 to 27.4 mBq per gram of dry tobacco for 210Po. The collective committed effective dose resulting from the use of cigarettes produced in Brazil per year is estimated to be 1.5 x 10(4) man-Sv. 相似文献
5.
The concentrations of natural radionuclides in surface soils around Adana, Turkey were determined using gamma ray spectrometry with an HPGe detector. The natural gamma ray radioactivity of the terrestrial radionuclides in air was calculated throughout different areas of Adana. The average activity concentrations of (238)U, (232)Th and (40)K were found to be 17.6, 21.1 and 297.5 Bq kg(-1), respectively. Outdoor gamma dose measurements in air 1m above ground level were determined by using a portable gamma scintillation detector. The gamma dose measurements in air were taken from the same places where soil samples were taken. Average outdoor gamma dose rates in sample stations were determined as 67 nGy h(-1). The annual effective dose to the public was found to be 82 microSv. 相似文献
6.
In this paper, an adaptation of a spectral profile analysis method, currently used in high-resolution spectrometry, to airborne gamma measurements is presented. A new algorithm has been developed for extraction of full absorption peaks by studying the variations in the spectral profile of data recorded with large-volume NaI detectors (16 l) with a short sampling time (2 s). The use of digital filters, taking into consideration the characteristics of the absorption peaks, significantly reduced the counting fluctuations, making detection possible based on study of the first and second derivatives. The absorption peaks are then obtained by modelling, followed by subtraction of the Compton continuum in the detection window. Compared to the conventional stripping ratio method, spectral profile analysis offers similar performance for the natural radioelements. The 137Cs 1SD detection limit is approximately 1200 Bq/m2 in a natural background of 200 Bq/kg 40K, 33 Bq/kg 238U and 33 Bq/kg 232Th. At low energy the very high continuum leads to detection limits similar to those obtained by the windows method, but the results obtained are more reliable. In the presence of peak overlaps, however, analysis of the spectral profile alone is not sufficient to separate the peaks, and further processing is necessary. Within the framework of environmental monitoring studies, spectral profile analysis is of great interest because it does not require any assumptions about the nature of the nuclides. The calculation of the concentrations from the results obtained is simple and reliable, since only the full absorption contributions are taken into consideration. A quantitative estimate of radioactive anomalies can thus be obtained rapidly. 相似文献
7.
The space blanket mitt which covered the Trek detector on Mir during four years of orbital flight has been measured for gamma radiation with HPGe and multidimensional spectrometers. Difference spectra from very-long-period spectrometer runs on the mitt and on a similar non-deployed mitt from the same manufacturer show that the mitt has acquired small but significant amounts of gamma radioactivity during orbital flight. Twelve gamma-ray peaks have been measured in the difference spectra, including peaks identified as due to 214Bi and 214Pb from the uranium-radium alpha decay series, and others possibly due to the uranium-actinium series. This implies the presence of a sparse population of uranium decay products in lower orbital space which can only have come from nuclear explosions, burned-up satellite nuclear batteries, the solar wind, or supernova fragments in the local interstellar medium. 相似文献
8.
Traces of the radionuclide (207)Bi were identified in soil and cryoconite (glacier sediment) samples from Alpine regions of Austria. This nuclide has been produced in thermonuclear explosions mainly in the early 1960s and subsequently dispersed in the atmosphere. Activity concentrations up to 22 Bq/kg d.m. have been found. The ratio (207)Bi:(137)Cs(global fallout) equals (1.70+/-0.12)10(-3), which is in accordance with literature data. When low levels of (207)Bi are assessed by gamma spectrometry, corrections must be made for a gamma line produced in the lead shield by neutron activation due to cosmic neutrons. 相似文献
9.
We describe a method for the determination of long-lived tin isotopes arising from nuclear fission. The isotopes are extracted from sediments with hydrochloric acid and separated by methylisobutylketone extraction, ion-exchange chromatography, precipitation of cesium hexachlorostannate and ferric hydroxide coprecipitation. The 100 000-year 126Sn was not detected but beta activity consistent with 121mSn (55 year) was found in sediment samples from a location known to be contaminated with fission products. 相似文献
10.
A computer code has been developed to simulate the gamma-ray spectra that would be measured by airborne gamma spectrometry (AGS) systems from sources containing short-lived fission products. The code uses simple numerical methods to simulate the production and decay of fission products and generates spectra for sodium iodide (NaI) detectors using Monte Carlo codes. A new Monte Carlo code using a virtual array of detectors to reduce simulation times for airborne geometries is described. Spectra generated for a short irradiation and laboratory geometry have been compared with an experimental data set. The agreement is good. Spectra have also been generated for airborne geometries and longer irradiation periods. The application of this code to generate AGS spectra for accident scenarios and their uses in the development and evaluation of spectral analysis methods for such situations are discussed. 相似文献
11.
The autoradiographic micromapping of rocks with various U and Th contents has been performed by means of CR-39 solid-state nuclear track detector (SSNTD). The optical track density was found to be highly correlated (r=0.92) with total alpha emitters activity calculated on the basis of field gamma spectrometric measurements of rock outcrops. The method was tested not only for the wide range activities of alpha emitters but various types of surface distribution (including highly radioactive mineral grains) as well. 相似文献
12.
Bиccлoвaнияx вoэмocy;жнocтeф пpимeн eния мeтoдoв coвaдeниф дффeктив нoгo cхeтa иэиuхaтeлeф пoхитpoнoв в б oльщиx oбpaэцax, pнpимeня жидкocт ныф cцинтлляциoнныф cхeтхик 4π для вceгo, cocтoяшиф иэ 2-x дeтeктocy;pныx кaмep 2π. Пpeждe вceгo иэuхaлocв oбpaэoвaниe фoн a, кaк oтвeтнaя peaция в мeтoдe co coвпaдeниф. B peэuлвтaтe импuлвcoв coвпaдeни ф в oбoиx дeтeктopныx кaмepax нaблю энaхитeлвныф uхacтoк фoнa. Иэuхaлacvcy; пoдaвлeни я фoнa пuтa cхeтa пueтa cхeтa aнт иcoвпaдeнeниф, нo этoт мeтoд нe oкaэaлcя uля uлu oхыхныx гaммa-иэлucy;хaтaeлeф. oднaк o, в cлнaяx, кoгпa в oбpaэцax coдepж aлиcв тaкиe иэлuхaтeли пoэитpoнoв, кaк 22Na и 58 co, фoн мoжнo былo энaхитeлвнo пoд aвитв и cхeтнuю cтaтиcтикu нa нa мнoгo юл юхшитв пpимeняя пpимeняя cпoco бы ы coвпaдeниф. Этoт мeтoд нe тoдвкo uмeнвщaeт фoн, нo тaкиe мoнoгaмм-иэлuхaтeли, кaк 137Cs 40К. Taким oбким oбpaэoм, этoт мeт oд нaпpaшивaeтcя caм coбoф для иэ peния иэлuхaтeлeф пoэитpoнoв в хeлoвeкe, гдe 137Cs 40К п pиcuтcтвuют, кaк интepфиpuюшиф фoн:. ZusammenfassungEin 4π-Flüssigkeits-“Ganzkörper”-Szintillationszähler, bestehend aus 2π-Detektrortanks wurde dazu verwendet, die mögliche Anwendung von Koinzidenzarbeitsweisen zur wirksamen Zählung von Positronenemittern in grossen Proben zu studieren. Zunächst wurde die Hintergrundemp-findlichkeit für die Koinzidenzform untersucht. Man beobachtete, dass ein ansehnlicher Teil des Hintergrundes von Impulsen in der Koinzidenz in beiden Detektortanks herrührte. Die Möglichkeit einer Unterdrückung des Hintergrundes durch Antikoinzidenzzählung wurde erforscht, aber dies stellte sich als unbrauchbar für eine Verbesserung der Zählstatistik zum Zählen gewöhnlicher Gammaemitter heraus. Wenn die Proben jedoch Positronenemitter wie 22Na and 58Co enthalten, so könnte der Hintergrund weitgehend unterdrückt und die Zählstatistik beträchtlich verbessert werden, wenn man Koinzidenzzählverfahren anwendet. Das Verfahren verminderte nicht nur den Hintergrund, sondern es diskriminierte auch gegenüber solchen Monogammaemittern wie 137Cs und 40K. Das Verfahren eignet sich somit zur Messung von Positronenemittern im Menschen, wo 137Cs und 40K als “Störhintergrund” zugegen sind. PDF (473 K)
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