为研究新型复合屏蔽材料的最佳厚度与各种成分最佳配比,用MCNP计算了中子、γ射线在稀土-高分子与重金属复合材料中的通量.对中子、γ射线在屏蔽体中变化规律进行了深入探索,同传统复合屏蔽材料的屏蔽性能进行了对比.结果表明,中子和γ射线通过屏蔽体时,其强度遵循指数衰减规律.新型屏蔽材料对中子的屏蔽效果均优于铅硼聚乙烯,对γ射线的屏蔽效果均劣于W-Ni合金,且并非稀土含量越高,材料对中子辐射屏蔽能力越强.
A series of shielding analyses have been performed to estimate the material composition and optimum thickness required for a new radiation shield with various rare-earth doped polymer and heavy metal mixtures.The neutron and y photon fluxes have been calculated by Monte Carlo N-Particle(MCNP) transport code.The results indicate that the relative fluxes of y photon and neutron in both traditional and new composite materials follow an exponential decay rule with the distance of penetration.It can be seen that the composite material consisting of rare-earth doped polymer and heavy metal has stronger neutron shielding performance than lead-boron polyethylene,but weaker y shielding effectiveness than W-Ni alloy.It isalso found that materials with more components of rare earth elements don't always provide better neutron shielding performance.
参考文献
[1] | Norman Morris Schaeffer.Reactor Shielding for Nuclear Engineers.Beijing:Atomic Energy Press,1983,285(in Chinese).(Norman Morris Schaeffer.核反应堆屏蔽工程学.北京:原子能出版社,1983,285.) |
[2] | Yang Wenfeng,Liu Ying,Yang Lin,et al.Materials Review,2007,21(5);82 (in Chinese).(杨文锋,刘颖,杨林,等.材料导报.2007,21(5):82.) |
[3] | Lv Jixin,Chen Jianting.Nuclear Power Engineering,1994,15:370(in Chinese).(吕继新,陈建廷.核动力工程,1994,15(4):370.) |
[4] | Leng Ruiping,Xie Jianlun.Number NCR38 Report:Neutron Radiation Protection.Beijing:Atomic Energy Press,1981.111 (in Chinese).(冷瑞平,谢建伦.NCRP38号报告:中子辐射的防护.北京:原子能出版社,1981.111.) |
[5] | Liu Li,Sun Chaohui,Wu Youping.China Synthetic Rubber Industry,2001,24:188(in Chinese).(刘力,孙朝晖,吴友平.合成橡胶工业,2001,240):188.) |
[6] | Ida K.Resin Composition Containing Rare Earth Element and Production thereof:Japan Kokai Tokky Koho,JP 60110756A2.1985. |
[7] | Los Alamos National Laboratory.MCNP-A General Monte Carlo N-Particle Transport Code.2000. |
- 下载量()
- 访问量()
- 您的评分:
-
10%
-
20%
-
30%
-
40%
-
50%