Endo S, Nitta Y, Ohtaki M, Takada J, Stepanenko V, Komatsu K, Tauchi H, Matsuura S, Iaskova E, Hoshi M
Research Institute for Radiation Biology and Medicine, Hiroshima University, Japan.
J Radiat Res. 1998 Sep;39(3):223-30. doi: 10.1269/jrr.39.223.
The dose absorbed fraction of rat thyroid by internal deposit of 131I has been calculated as a function of effective diameter of thyroid. The calculations were done using two types of Monte Carlo simulations: one was by a simple energy-loss calculation in spherical volume according to the electron stopping power, and another by a more realistic simulation using Monte Carlo N-Particle Transport code system Version 4A (MCNP). These two calculations were consistent with each other within a deviation of 5%. The absorbed fractions in spherical thyroid were drastically changed up to 5 mm diameter, and then almost all energy was deposited within 10 mm diameter. For the practical application to the animal experiment, the absorbed fractions of ellipsoid-shaped thyroids were also calculated for 1-, 4- and 9-week-old rats, where the fractions were estimated to be 0.61, 0.67 and 0.68, respectively. It was also found that the absorbed fraction of the ellipsoid with various dimensions can be simulated by a calculation for spherical volume with a comparable effective diameter.
已计算出¹³¹I 体内沉积时大鼠甲状腺的剂量吸收分数与甲状腺有效直径的函数关系。计算使用了两种蒙特卡罗模拟方法:一种是根据电子阻止本领在球形体积内进行简单的能量损失计算,另一种是使用蒙特卡罗 N 粒子输运代码系统版本 4A(MCNP)进行更实际的模拟。这两种计算结果在 5%的偏差范围内相互一致。球形甲状腺的吸收分数在直径达 5 毫米时急剧变化,然后几乎所有能量都沉积在直径 10 毫米范围内。为了实际应用于动物实验,还计算了 1 周龄、4 周龄和 9 周龄大鼠椭圆形甲状腺的吸收分数,其值分别估计为 0.61、0.67 和 0.68。还发现,具有不同尺寸的椭球体的吸收分数可以通过具有可比有效直径的球形体积计算来模拟。