Biggs Peter J, Styczynski John R
Department of Radiation Oncology, Massachusetts General Hospital, Harvard Medical School, Boston, MA 02114, USA.
Health Phys. 2008 Oct;95(4):425-32. doi: 10.1097/01.HP.0000319905.27506.88.
The angle of obliquity is used in radiation shielding calculations to account for the longer path length x rays will see when obliquely incident on the protective barrier. According to the National Council on Radiation Protection and Measurements (NCRP), use of the angle of obliquity is explicitly assumed for primary radiation, so that an angle of obliquity for secondary radiation is never addressed. However, in the example section of the latest report, it specifically recommends against using an angle of obliquity for scattered radiation. To check this assumption, the existence or not of an angle of obliquity for scattered radiation has been investigated for bremsstrahlung x-ray beams of 4, 6, 10, 15, and 18 MV and for barriers consisting of concrete, lead, and steel using a Monte Carlo approach. The MCNP Monte Carlo code, v4.2C, has been used to generate scattered radiation at 30 degrees from a water phantom and incident on a secondary barrier at the same angle relative to the normal to the barrier. The barrier thickness was increased from zero to a thickness sufficient to reduce the fluence (f4 tally) to <10(-3). A transmission curve was created for each energy-barrier material combination by normalizing to zero thickness. The results for the first tenth-value layer (TVL) in concrete (5 energies) show an average angle of obliquity of 21.7 degrees +/- 5.6 degrees , and for the first two TVLs averaged 29.7 degrees +/- 3.9 degrees . The results for the first TVL in lead (3 energies) show an average angle of obliquity of 27.7 degrees +/- 4.0 degrees , and for the first two TVLs averaged 20.5 degrees +/- 5.8 degrees . There are no data in the NCRP reports for 30 degrees scattered radiation attenuated by steel with which to make a comparison.
倾斜角用于辐射屏蔽计算,以考虑X射线斜入射到防护屏障时所经过的较长路径长度。根据美国国家辐射防护与测量委员会(NCRP)的规定,对于初级辐射明确假定使用倾斜角,因此从未涉及次级辐射的倾斜角问题。然而,在最新报告的示例部分,特别建议不要对散射辐射使用倾斜角。为检验这一假设,已采用蒙特卡罗方法研究了4、6、10、15和18 MV的轫致辐射X射线束以及由混凝土、铅和钢构成的屏障的散射辐射倾斜角的存在与否。使用MCNP蒙特卡罗代码v4.2C从水模体产生30度的散射辐射,并以相对于屏障法线相同的角度入射到次级屏障上。屏障厚度从零增加到足以将注量(f4计数)降低至<10(-3)的厚度。通过归一化为零厚度,为每种能量-屏障材料组合创建了一条传输曲线。混凝土中前十分之一值层(TVL)(5种能量)的结果显示平均倾斜角为21.7度±5.6度,前两个TVL的平均值为29.7度±3.9度。铅中前TVL(3种能量)的结果显示平均倾斜角为27.7度±4.0度,前两个TVL的平均值为20.5度±5.8度。NCRP报告中没有关于30度散射辐射被钢衰减的数据可供比较。