{"title":"放射性核素微分布对辐射防护建议限值的影响,一个模型。","authors":"L E Feinendegen, E P Cronkite","doi":"","DOIUrl":null,"url":null,"abstract":"<p><p>The heterogeneous distribution and accumulation of radionuclides in discrete areas of cellular and subcellular dimensions is called microdistribution. The biological effect of microdistributed radionuclides with low-range emissions is determined by the degree of irradiation of the radiosensitive microareas of the body. The critical microareas of the body are nuclei of such cells which (1) are radiosensitive, (2) are essential to maintaining life, (3) are irreplaceable, (4) have a long life span and/or renew themselves. In this sense, the stem cell nuclei are considered critical microareas of the body. Stem cells constitute only a small fraction of the total body's cellularity. In case of concentration of radionuclides in stem cell nuclei, such as from incorporated labeled DNA precursors, there is a total congruence of the radionuclide microdistribution with the radiosensitive microarea, and the biological effect is expected to be enhanced over that from a homogeneous distribution of the same amount of radionuclides. This situation is discussed for 3H, 14C and 125I incorporate into mice as tracers of DNA precursors. The average labeling intensity of the bone marrow cell nucleus was taken to represent the average labeling intensity of the stem cell nucleus. The dose to the stem cell nucleus, then, is derived from the number and energy of decays originating in the nuclear mass of 270 X 10(-12) g. The transmutation effect from isotopic decay in DNA is considered in order to arrive at dose equivalents. On the basis of known data on labeling efficiency of bone marrow and on stem cell proliferation kinetics in the mouse, the infinite accumulation of decays in and the total expected dose to the stem cell nucleus was calculated for intravenous injection or ingestion of 1 muCi 3H-TdR per g body weight. The distribution factor and an annual limit on intake for the mouse model was suggested. Corresponding data are presented for 14C-TdR and 125I-UdR. A special situation is given for the case of hot particles where there is a random relationship between microdistributed radionuclides and critical microareas of the body. In this instance, theory predicts a decreased biological effect in comparison to the situation where the same amount of radionuclides is homogeneously distributed. There is experimental evidence that supports the theoretical predictions particularly for the case of 236Pu dioxide in the human lung.</p>","PeriodicalId":75768,"journal":{"name":"Current topics in radiation research quarterly","volume":"12 1-4","pages":"83-99"},"PeriodicalIF":0.0000,"publicationDate":"1978-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Effect of microdistribution of radionuclides on recommended limits in radiation protection, a model.\",\"authors\":\"L E Feinendegen, E P Cronkite\",\"doi\":\"\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>The heterogeneous distribution and accumulation of radionuclides in discrete areas of cellular and subcellular dimensions is called microdistribution. The biological effect of microdistributed radionuclides with low-range emissions is determined by the degree of irradiation of the radiosensitive microareas of the body. The critical microareas of the body are nuclei of such cells which (1) are radiosensitive, (2) are essential to maintaining life, (3) are irreplaceable, (4) have a long life span and/or renew themselves. In this sense, the stem cell nuclei are considered critical microareas of the body. Stem cells constitute only a small fraction of the total body's cellularity. In case of concentration of radionuclides in stem cell nuclei, such as from incorporated labeled DNA precursors, there is a total congruence of the radionuclide microdistribution with the radiosensitive microarea, and the biological effect is expected to be enhanced over that from a homogeneous distribution of the same amount of radionuclides. This situation is discussed for 3H, 14C and 125I incorporate into mice as tracers of DNA precursors. The average labeling intensity of the bone marrow cell nucleus was taken to represent the average labeling intensity of the stem cell nucleus. The dose to the stem cell nucleus, then, is derived from the number and energy of decays originating in the nuclear mass of 270 X 10(-12) g. The transmutation effect from isotopic decay in DNA is considered in order to arrive at dose equivalents. On the basis of known data on labeling efficiency of bone marrow and on stem cell proliferation kinetics in the mouse, the infinite accumulation of decays in and the total expected dose to the stem cell nucleus was calculated for intravenous injection or ingestion of 1 muCi 3H-TdR per g body weight. The distribution factor and an annual limit on intake for the mouse model was suggested. Corresponding data are presented for 14C-TdR and 125I-UdR. A special situation is given for the case of hot particles where there is a random relationship between microdistributed radionuclides and critical microareas of the body. In this instance, theory predicts a decreased biological effect in comparison to the situation where the same amount of radionuclides is homogeneously distributed. There is experimental evidence that supports the theoretical predictions particularly for the case of 236Pu dioxide in the human lung.</p>\",\"PeriodicalId\":75768,\"journal\":{\"name\":\"Current topics in radiation research quarterly\",\"volume\":\"12 1-4\",\"pages\":\"83-99\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1978-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Current topics in radiation research quarterly\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Current topics in radiation research quarterly","FirstCategoryId":"1085","ListUrlMain":"","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
放射性核素在细胞和亚细胞尺度上的不均匀分布和积累称为微分布。低范围放射的微分布放射性核素的生物效应是由人体放射敏感微区的辐照程度决定的。人体的关键微区是这些细胞的细胞核,这些细胞(1)对辐射敏感,(2)对维持生命至关重要,(3)不可替代,(4)寿命长和/或自我更新。从这个意义上说,干细胞核被认为是人体的关键微区。干细胞只占人体细胞总数的一小部分。在干细胞核中的放射性核素浓度的情况下,例如来自掺入标记的DNA前体,放射性核素微分布与辐射敏感微区完全一致,并且预计比相同数量的放射性核素均匀分布的生物效应更强。讨论了3H、14C和125I作为DNA前体示踪剂掺入小鼠体内的情况。取骨髓细胞核的平均标记强度代表干细胞细胞核的平均标记强度。因此,对干细胞细胞核的剂量由源自270 X 10(-12) g核质量的衰变的数量和能量得出。为了达到当量剂量,考虑了DNA中同位素衰变的嬗变效应。根据已知的小鼠骨髓标记效率和干细胞增殖动力学数据,计算每g体重静脉注射或摄入1 muCi 3H-TdR时,衰变在干细胞细胞核内的无限累积量和总预期剂量。提出了小鼠模型的分布因子和年摄食量限制。给出了14C-TdR和125I-UdR的相应数据。在热粒子的情况下,微分布的放射性核素与身体的临界微区之间存在随机关系,这是一种特殊的情况。在这种情况下,理论预测,与相同数量的放射性核素均匀分布的情况相比,生物效应会降低。有实验证据支持理论预测,特别是对人体肺部二氧化236Pu的情况。
Effect of microdistribution of radionuclides on recommended limits in radiation protection, a model.
The heterogeneous distribution and accumulation of radionuclides in discrete areas of cellular and subcellular dimensions is called microdistribution. The biological effect of microdistributed radionuclides with low-range emissions is determined by the degree of irradiation of the radiosensitive microareas of the body. The critical microareas of the body are nuclei of such cells which (1) are radiosensitive, (2) are essential to maintaining life, (3) are irreplaceable, (4) have a long life span and/or renew themselves. In this sense, the stem cell nuclei are considered critical microareas of the body. Stem cells constitute only a small fraction of the total body's cellularity. In case of concentration of radionuclides in stem cell nuclei, such as from incorporated labeled DNA precursors, there is a total congruence of the radionuclide microdistribution with the radiosensitive microarea, and the biological effect is expected to be enhanced over that from a homogeneous distribution of the same amount of radionuclides. This situation is discussed for 3H, 14C and 125I incorporate into mice as tracers of DNA precursors. The average labeling intensity of the bone marrow cell nucleus was taken to represent the average labeling intensity of the stem cell nucleus. The dose to the stem cell nucleus, then, is derived from the number and energy of decays originating in the nuclear mass of 270 X 10(-12) g. The transmutation effect from isotopic decay in DNA is considered in order to arrive at dose equivalents. On the basis of known data on labeling efficiency of bone marrow and on stem cell proliferation kinetics in the mouse, the infinite accumulation of decays in and the total expected dose to the stem cell nucleus was calculated for intravenous injection or ingestion of 1 muCi 3H-TdR per g body weight. The distribution factor and an annual limit on intake for the mouse model was suggested. Corresponding data are presented for 14C-TdR and 125I-UdR. A special situation is given for the case of hot particles where there is a random relationship between microdistributed radionuclides and critical microareas of the body. In this instance, theory predicts a decreased biological effect in comparison to the situation where the same amount of radionuclides is homogeneously distributed. There is experimental evidence that supports the theoretical predictions particularly for the case of 236Pu dioxide in the human lung.