Theoretical study for the calculation of some attenuation parameters of polymeric composites

Suham Asad Maykhan, A. Mkhaiber
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Abstract

In this research, the attenuation of gamma rays for different materials was studied. Some composite materials, which have desirable properties by workers in different fields especially shielding, have been used. Polyethylene (P.E.) was used as the base material and (BH3O3),(CaSO6H4),(Bi2GeO3) as reinforcement materials with various concentrations (10,20,30,40 and 50) wt% at different energies (0.5,1,2,3,4 and 5)MeV.Through this research we study the total attenuation coefficient (µ), effective atomic number Zeff and half thickness.Through the study we note that the Zeff and linear attenuation coefficient(µ) rise with rising concentration of reinforcement materials, while the half thickness reduce by rising the concentration of reinforcement materials. As a result, the linear attenuation coefficient (µ) and Zeff reduce by rising the energy of the gamma rays, While the Half value layer increases with energy. Total linear attenuation coefficient (µ) was calculated by theprogram Xcom.In this research, the attenuation of gamma rays for different materials was studied. Some composite materials, which have desirable properties by workers in different fields especially shielding, have been used. Polyethylene (P.E.) was used as the base material and (BH3O3),(CaSO6H4),(Bi2GeO3) as reinforcement materials with various concentrations (10,20,30,40 and 50) wt% at different energies (0.5,1,2,3,4 and 5)MeV.Through this research we study the total attenuation coefficient (µ), effective atomic number Zeff and half thickness.Through the study we note that the Zeff and linear attenuation coefficient(µ) rise with rising concentration of reinforcement materials, while the half thickness reduce by rising the concentration of reinforcement materials. As a result, the linear attenuation coefficient (µ) and Zeff reduce by rising the energy of the gamma rays, While the Half value layer increases with energy. Total linear attenuation coefficient (µ) was calculated by theprogram Xcom.
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高分子复合材料若干衰减参数计算的理论研究
在本研究中,研究了不同材料对伽马射线的衰减。一些复合材料在不同的领域,尤其是屏蔽领域,已经得到了广泛的应用。以聚乙烯(pe)为基材,以(BH3O3)、(CaSO6H4)、(Bi2GeO3)为增强材料,在不同能量(0.5、1、2、3、4和5)MeV下,以不同的浓度(10、20、30、40和50)wt%。通过本研究,我们研究了总衰减系数(µ)、有效原子序数Zeff和半厚度。通过研究我们发现,随着增强材料浓度的增加,Zeff和线性衰减系数(µ)增加,而半厚度随着增强材料浓度的增加而减小。结果表明,线性衰减系数(µ)和Zeff随伽马射线能量的增加而减小,而半值层随能量的增加而增大。总线性衰减系数(µ)由Xcom程序计算。在本研究中,研究了不同材料对伽马射线的衰减。一些复合材料在不同的领域,尤其是屏蔽领域,已经得到了广泛的应用。以聚乙烯(pe)为基材,以(BH3O3)、(CaSO6H4)、(Bi2GeO3)为增强材料,在不同能量(0.5、1、2、3、4和5)MeV下,以不同的浓度(10、20、30、40和50)wt%。通过本研究,我们研究了总衰减系数(µ)、有效原子序数Zeff和半厚度。通过研究我们发现,随着增强材料浓度的增加,Zeff和线性衰减系数(µ)增加,而半厚度随着增强材料浓度的增加而减小。结果表明,线性衰减系数(µ)和Zeff随伽马射线能量的增加而减小,而半值层随能量的增加而增大。总线性衰减系数(µ)由Xcom程序计算。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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