{"title":"320 keV光子宽光束几何结构窄光束衰减系数的测定","authors":"H.A. Jahagirdar, B. Hanumaiah, S.R. Thontadarya","doi":"10.1016/0883-2889(92)90180-M","DOIUrl":null,"url":null,"abstract":"<div><p>Narrow beam mass attenuation coefficients, μ/ρ, of 320 keV photons, emitted from the <sup>51</sup>Cr radioisotope have been measured in various high <em>Z</em> materials such as Pb; BiPO<sub>4</sub>; (CH<sub>3</sub>COO)<sub>2</sub>·Pb·3H<sub>2</sub>O; Pb(NO<sub>3</sub>)<sub>2</sub>; Na<sub>2</sub>WO<sub>4</sub>·2H<sub>2</sub>O, using a broad beam geometrical configuration, employing a 2′' × 1′' (5.1 <em>cm</em> × 2.54 <em>cm</em>) (0.051 <em>m</em> × 0.025 <em>m</em>) NaI (Tl) detector spectrometer system coupled to a 1 k multichannel analyser. The measured μ/ρ values in cm<sup>2</sup>/g for the above materials in the transmission range from 50% to 20% respectively are 0.34 ± 0.01 (0.35); 0.295 ± 0.002 (0.30); 0.23 ± 0.01 (0.24); 0.256 ± 0.003 (0.26); 0.255 ± 0.003 (0.256). The values given in parentheses are estimated theoretically from the mixture rule using tabulated values of Hubbell (1982). It is observed that for high <em>Z</em> compounds at low energies, the exponential law of attenuation will be valid even for a broad beam set up in the transmission range from 50% to 20%. The attenuation coefficients of elements derived from this method agree fairly well with the tabulated narrow beam attenuation coefficients indicating the validity of the mixture rule in this region of transmission.</p></div>","PeriodicalId":14288,"journal":{"name":"International Journal of Radiation Applications and Instrumentation. Part A. Applied Radiation and Isotopes","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"1992-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0883-2889(92)90180-M","citationCount":"21","resultStr":"{\"title\":\"Determination of narrow beam attenuation coefficients from a broad beam geometrical configuration for 320 keV photons\",\"authors\":\"H.A. Jahagirdar, B. Hanumaiah, S.R. Thontadarya\",\"doi\":\"10.1016/0883-2889(92)90180-M\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Narrow beam mass attenuation coefficients, μ/ρ, of 320 keV photons, emitted from the <sup>51</sup>Cr radioisotope have been measured in various high <em>Z</em> materials such as Pb; BiPO<sub>4</sub>; (CH<sub>3</sub>COO)<sub>2</sub>·Pb·3H<sub>2</sub>O; Pb(NO<sub>3</sub>)<sub>2</sub>; Na<sub>2</sub>WO<sub>4</sub>·2H<sub>2</sub>O, using a broad beam geometrical configuration, employing a 2′' × 1′' (5.1 <em>cm</em> × 2.54 <em>cm</em>) (0.051 <em>m</em> × 0.025 <em>m</em>) NaI (Tl) detector spectrometer system coupled to a 1 k multichannel analyser. The measured μ/ρ values in cm<sup>2</sup>/g for the above materials in the transmission range from 50% to 20% respectively are 0.34 ± 0.01 (0.35); 0.295 ± 0.002 (0.30); 0.23 ± 0.01 (0.24); 0.256 ± 0.003 (0.26); 0.255 ± 0.003 (0.256). The values given in parentheses are estimated theoretically from the mixture rule using tabulated values of Hubbell (1982). It is observed that for high <em>Z</em> compounds at low energies, the exponential law of attenuation will be valid even for a broad beam set up in the transmission range from 50% to 20%. The attenuation coefficients of elements derived from this method agree fairly well with the tabulated narrow beam attenuation coefficients indicating the validity of the mixture rule in this region of transmission.</p></div>\",\"PeriodicalId\":14288,\"journal\":{\"name\":\"International Journal of Radiation Applications and Instrumentation. Part A. Applied Radiation and Isotopes\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1992-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0883-2889(92)90180-M\",\"citationCount\":\"21\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal of Radiation Applications and Instrumentation. Part A. Applied Radiation and Isotopes\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/088328899290180M\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Radiation Applications and Instrumentation. Part A. Applied Radiation and Isotopes","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/088328899290180M","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 21
摘要
在各种高Z物质(如Pb)中测量了51Cr放射性同位素发射的320 keV光子的窄束质量衰减系数μ/ρ;BiPO4;(CH3COO) 2·3 Pb·h2o;Pb(3号)2;Na2WO4·2H2O,采用宽光束几何结构,采用2“× 1”(5.1 cm × 2.54 cm) (0.051 m × 0.025 m) NaI (Tl)探测器光谱仪系统与1 k多通道分析仪耦合。上述材料在50% ~ 20%透射率范围内测得μ/ρ值(cm2/g)分别为0.34±0.01 (0.35);0.295±0.002 (0.30);0.23±0.01 (0.24);0.256±0.003 (0.26);0.255±0.003(0.256)。括号内给出的值是使用Hubbell(1982)的表列值从混合规则理论上估计的。我们观察到,对于低能量的高Z化合物,即使在50% ~ 20%的传输范围内设置宽光束,衰减的指数定律仍然有效。该方法得到的单元衰减系数与表列的窄波束衰减系数吻合较好,表明混合规则在该传输区域的有效性。
Determination of narrow beam attenuation coefficients from a broad beam geometrical configuration for 320 keV photons
Narrow beam mass attenuation coefficients, μ/ρ, of 320 keV photons, emitted from the 51Cr radioisotope have been measured in various high Z materials such as Pb; BiPO4; (CH3COO)2·Pb·3H2O; Pb(NO3)2; Na2WO4·2H2O, using a broad beam geometrical configuration, employing a 2′' × 1′' (5.1 cm × 2.54 cm) (0.051 m × 0.025 m) NaI (Tl) detector spectrometer system coupled to a 1 k multichannel analyser. The measured μ/ρ values in cm2/g for the above materials in the transmission range from 50% to 20% respectively are 0.34 ± 0.01 (0.35); 0.295 ± 0.002 (0.30); 0.23 ± 0.01 (0.24); 0.256 ± 0.003 (0.26); 0.255 ± 0.003 (0.256). The values given in parentheses are estimated theoretically from the mixture rule using tabulated values of Hubbell (1982). It is observed that for high Z compounds at low energies, the exponential law of attenuation will be valid even for a broad beam set up in the transmission range from 50% to 20%. The attenuation coefficients of elements derived from this method agree fairly well with the tabulated narrow beam attenuation coefficients indicating the validity of the mixture rule in this region of transmission.