Comparison of finite element modeling and Monte Carlo simulations for interstitial photodynamic therapy (Conference Presentation)

Emily Oakley, A. Manalac, Jeffrey Cassidy, L. Lilge, G. Shafirstein
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Abstract

Background and Objectives: Finite Element Methods (FEM) and Monte Carlo (MC, FullMonte) simulations are employed to compute light propagation during interstitial photodynamic therapy. FullMonte models the light source as a fixed number of photons emitted from the center of the catheter. In the FEM, the light source is modeled as a flux of photons emitted from the outside diameter of the catheter. The objective of this study was to compare the FEM and MC computed light fluence rate distributions. Methods: A solid phantom with tissue optical properties was used to compare MC simulations conducted using FullMonte and FEM using COMSOL Multiphysics. A tetrahedral mesh of approximately 400,000 elements was created to mimic experiments in the phantom with one central 2 cm cylindrical diffuser fiber, and five IP85 detector fibers were inserted 5, 10, 15, 20, and 25 mm from the light source. FEM and FullMonte simulations were conducted for 50 and 100 mW/cm source power, and the resulting fluence rates were compared, at the detector locations. Results: Initially, the computed fluence rates differed significantly between the MC and FEM simulations. However, the light gradient was comparable between both methods. Changing the FEM boundary conditions such that the light source was modeled as a flux of photons emitted from inside the catheter approximately 0.6 mm from the outside diameter resulted in a better agreement (16% difference). Conclusions: The light source boundary condition is a major contributor to the difference between FEM and FullMonte computed light distributions. Acknowledgements: This work was supported in part by National Cancer Institute of the National Institutes of Health under Award Number R01CA193610 to G. Shafirstein
间质性光动力治疗的有限元模拟与蒙特卡罗模拟的比较(会议报告)
背景与目的:采用有限元法(FEM)和蒙特卡罗(MC, FullMonte)模拟计算间隙光动力治疗过程中的光传播。FullMonte将光源建模为从导管中心发射的固定数量的光子。在FEM中,光源被建模为从导管外径发射的光子通量。本研究的目的是比较FEM和MC计算的光通量分布。方法:采用具有组织光学特性的实体幻影,比较FullMonte和COMSOL Multiphysics模拟的MC模拟结果。一个大约400,000个元件的四面体网格被创建来模拟实验,其中一个中央2厘米的圆柱形扩散光纤,五个IP85探测器光纤分别插入距离光源5、10、15、20和25毫米。在50和100 mW/cm的源功率下进行了FEM和FullMonte模拟,并在探测器位置比较了所得的通量率。结果:最初,MC和FEM模拟计算的通量率有显著差异。然而,两种方法之间的光梯度具有可比性。改变FEM边界条件,将光源建模为从导管内部发射的光子通量,距离外径约0.6 mm,结果更符合(相差16%)。结论:光源边界条件是造成有限元法与FullMonte法计算光分布差异的主要因素。致谢:这项工作得到了美国国立卫生研究院国家癌症研究所的部分支持,奖励号为R01CA193610,授予G. Shafirstein
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