{"title":"治疗性质子同步加速器辐射防护优化研究","authors":"Weiguo Zhu, Jing Liang, Chang-song Hou, Dexing Lian, Zhen Zhang","doi":"10.3760/CMA.J.ISSN.0254-5098.2019.09.013","DOIUrl":null,"url":null,"abstract":"Objective \nTo investigate the effect of iron shield at different depths within main protection wall on the dose rate outside the protection wall. \n \n \nMethods \nBy adopting the FLUKA code, a therapeutic room model was constructed with its primary protective barrier consisting of concrete and iron. In order to obtain its ambient dose equivalent rate distribution, the 250 MeV protons and 220 MeV protons impinging on water phantom were simulated separately. \n \n \nResults \nWith varying depth of iron plate embedded in barrier, the ambient dose equivalent rates in the two simulated conditions differed sinificantly at 30 cm outside the protection wall. The maximum ambient dose equivalent rate(220 MeV: 3.42 μSv/h, 250 MeV: 6.39 μSv/h) was more than 2 times higher than the minimum ambient dose equivalent rate(220 MeV: 1.75 μSv/h, 250 MeV: 3.32 μSv/h). \n \n \nConclusions \nIn the design of therapeutic proton accelerator, it is essential to evaluate carefully the location where the iron shield is in main protection wall. \n \n \nKey words: \nMonte Carlo simulation; Therapeutic proton accelerator; Barrier; Ambient dose equivalent rate","PeriodicalId":36403,"journal":{"name":"中华放射医学与防护杂志","volume":"271 1","pages":"707-710"},"PeriodicalIF":0.0000,"publicationDate":"2019-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Study on the optimization of radiation protection for therapeutic proton synchrotron\",\"authors\":\"Weiguo Zhu, Jing Liang, Chang-song Hou, Dexing Lian, Zhen Zhang\",\"doi\":\"10.3760/CMA.J.ISSN.0254-5098.2019.09.013\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Objective \\nTo investigate the effect of iron shield at different depths within main protection wall on the dose rate outside the protection wall. \\n \\n \\nMethods \\nBy adopting the FLUKA code, a therapeutic room model was constructed with its primary protective barrier consisting of concrete and iron. In order to obtain its ambient dose equivalent rate distribution, the 250 MeV protons and 220 MeV protons impinging on water phantom were simulated separately. \\n \\n \\nResults \\nWith varying depth of iron plate embedded in barrier, the ambient dose equivalent rates in the two simulated conditions differed sinificantly at 30 cm outside the protection wall. The maximum ambient dose equivalent rate(220 MeV: 3.42 μSv/h, 250 MeV: 6.39 μSv/h) was more than 2 times higher than the minimum ambient dose equivalent rate(220 MeV: 1.75 μSv/h, 250 MeV: 3.32 μSv/h). \\n \\n \\nConclusions \\nIn the design of therapeutic proton accelerator, it is essential to evaluate carefully the location where the iron shield is in main protection wall. \\n \\n \\nKey words: \\nMonte Carlo simulation; Therapeutic proton accelerator; Barrier; Ambient dose equivalent rate\",\"PeriodicalId\":36403,\"journal\":{\"name\":\"中华放射医学与防护杂志\",\"volume\":\"271 1\",\"pages\":\"707-710\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-09-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"中华放射医学与防护杂志\",\"FirstCategoryId\":\"3\",\"ListUrlMain\":\"https://doi.org/10.3760/CMA.J.ISSN.0254-5098.2019.09.013\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"Medicine\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"中华放射医学与防护杂志","FirstCategoryId":"3","ListUrlMain":"https://doi.org/10.3760/CMA.J.ISSN.0254-5098.2019.09.013","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"Medicine","Score":null,"Total":0}
Study on the optimization of radiation protection for therapeutic proton synchrotron
Objective
To investigate the effect of iron shield at different depths within main protection wall on the dose rate outside the protection wall.
Methods
By adopting the FLUKA code, a therapeutic room model was constructed with its primary protective barrier consisting of concrete and iron. In order to obtain its ambient dose equivalent rate distribution, the 250 MeV protons and 220 MeV protons impinging on water phantom were simulated separately.
Results
With varying depth of iron plate embedded in barrier, the ambient dose equivalent rates in the two simulated conditions differed sinificantly at 30 cm outside the protection wall. The maximum ambient dose equivalent rate(220 MeV: 3.42 μSv/h, 250 MeV: 6.39 μSv/h) was more than 2 times higher than the minimum ambient dose equivalent rate(220 MeV: 1.75 μSv/h, 250 MeV: 3.32 μSv/h).
Conclusions
In the design of therapeutic proton accelerator, it is essential to evaluate carefully the location where the iron shield is in main protection wall.
Key words:
Monte Carlo simulation; Therapeutic proton accelerator; Barrier; Ambient dose equivalent rate