Schnerr Roald S, de Jong Anouk N, Landry Guillaume, Jeukens Cécile R L P N, Wierts Roel
Department of Radiology, Maastricht UMC+, 6229 HX, Maastricht, The Netherlands.
Department of Medical Physics, Amphia Ziekenhuis, 4818 CK, Breda, The Netherlands.
Med Phys. 2017 Mar;44(3):1113-1119. doi: 10.1002/mp.12113.
In the design of nuclear medicine treatment and examination rooms, an important consideration is the shielding required for ionizing radiation from the radioactive isotopes used. The shielding in the walls is normally limited to a height lower than the actual ceiling height. The direct radiation, possibly with build-up correction, can be calculated relatively easily. However, little data are available to estimate the dose contribution from ionizing radiation traveling over the wall shielding and scattering off the ceiling. We aim to determine the contribution of the ceiling scatter to the radiation dose outside nuclear medicine rooms.
Monte Carlo simulations were performed using Gate for different heights of lead shielding in the wall, and different ceiling heights. A point source in air of Tc (141 keV), I (365 keV) or F (511 keV) was placed 1.0 m above the floor, 3.0 m from the lead shielding. Simulations of ceiling scatter only and for the total radiation dose were performed for these 3 isotopes, 5 different ceiling heights and 4-8 different wall shielding heights, resulting in a total of 165 simulations. This allowed us to compare the contribution of the radiation passing through the shielding and the ceiling scatter.
We find that the shielding required for the primary radiation, measured in half-value layers, is an important factor in determining the relative contribution of ceiling scatter. When more than about 4 half-value layers of shielding are used, ceiling scatter becomes the dominant factor and should be taken into account in the shielding design. In many practical cases for low energy photons (e.g. from Tc; 141 keV; half-value layer of 0.26 mm lead), 2 mm of lead is used and ceiling scatter is a dominating factor contributing >~70% of the dose outside the shielded room. For higher energies (e.g. F; 511 keV; half-value layer of 3.9 mm lead) the ceiling scatter is typically less than about 15% when 8 mm of lead shielding is used.
We have performed simulations that allow an estimation of the contribution of ceiling scatter to the radiation dose outside a room, based on the ceiling height, shielding height, and isotope used. This will allow for improved shielding designs in nuclear medicine departments.
在核医学治疗和检查室的设计中,一个重要的考虑因素是对所用放射性同位素产生的电离辐射所需的屏蔽。墙壁的屏蔽通常限制在低于实际天花板高度的位置。直接辐射,可能经过积累修正后,相对容易计算。然而,几乎没有数据可用于估计穿过墙壁屏蔽并从天花板散射的电离辐射的剂量贡献。我们旨在确定天花板散射对核医学房间外辐射剂量的贡献。
使用Gate对墙壁中不同高度的铅屏蔽和不同的天花板高度进行蒙特卡罗模拟。在离铅屏蔽3.0米、高于地面1.0米处的空气中放置一个(^{99m}Tc)(141 keV)、(^{131}I)(365 keV)或(^{18}F)(511 keV)的点源。对这3种同位素、5种不同的天花板高度和4 - 8种不同的墙壁屏蔽高度进行仅天花板散射和总辐射剂量的模拟,总共进行了165次模拟。这使我们能够比较穿过屏蔽的辐射和天花板散射的贡献。
我们发现,以半价层衡量的初级辐射所需屏蔽是确定天花板散射相对贡献的一个重要因素。当使用超过约4个半价层的屏蔽时,天花板散射成为主导因素,在屏蔽设计中应予以考虑。在许多低能光子的实际情况中(例如来自(^{99m}Tc);141 keV;铅的半价层为0.26毫米),使用2毫米的铅,天花板散射是主导因素,对屏蔽室外剂量的贡献超过约70%。对于更高能量(例如(^{18}F);511 keV;铅的半价层为3.9毫米),当使用8毫米的铅屏蔽时,天花板散射通常小于约15%。
我们进行的模拟能够根据天花板高度、屏蔽高度和所用同位素来估计天花板散射对房间外辐射剂量的贡献。这将有助于改进核医学科室的屏蔽设计。