毫米波下真实组织模型的面积平均吸收功率密度评估

A. Kapetanović, G. Sacco, D. Poljak, M. Zhadobov
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引用次数: 1

摘要

目前,大多数最先进的计算剂量学研究利用平面组织模型来简化问题的几何形状,从而降低计算复杂性。然而,根据穿透深度和曲率半径的比例,这可能导致由于相消干涉而导致组织吸收功率的不正确估计。在本研究中,我们通过计算吸收功率密度矢量场的法向分量的表面积分,提出了一种精确评估弯曲组织等效模型中面积平均吸收功率密度的方法。对60 GHz频率下耳模型的平面波暴露进行了数值分析。我们还研究了平均面积形状对吸收功率密度的影响,考虑了1 cm2的正方形和圆盘形平均表面。结果表明,横向电极化和横向磁极化在圆盘状平均表面上的面积平均吸收功率密度存在14%的相对差异,参考值为平面均匀模型和法向入射的面积平均吸收功率密度值。在相同的参考值下,当平均面积形状改变时,横向电极化和横向磁极化的差异分别为1.81%和0.92%,可以忽略不计。根据所研究的暴露场景,面积平均吸收功率密度随平均表面几何形状的变化不如与入射场极化有关的变化显著。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Assessment of Area-Average Absorbed Power Density on Realistic Tissue Models at mmWaves
Currently, most state-of-the-art research in computational dosimetry utilizes flat-surface tissue models to simplify the problem geometry and thus mitigate computational complexity. However, depending on the ratio of the penetration depth and the curvature radius, this may lead to a non-correct estimation of the power absorbed by the tissues due to constructive/destructive interference. In this study, we propose an accurate evaluation of the area-average absorbed power density in curved tissue-equivalent models by computing the surface integral of the normal component of the absorbed power density vector field. The numerical analysis is performed for plane wave exposure of an ear model at 60 GHz. We also investigate the effect of the averaging area shape on the absorbed power density by considering 1 cm2 square- and disk-shaped averaging surfaces. Results show a substantial relative difference of 14 % in the area-averaged absorbed power density over a disk-shaped averaging surface between transverse electric and magnetic polarization, with the reference being the value of the area-averaged absorbed power density for a planar homogeneous model and normal incidence. By using the same reference value, negligible differences of 1.81 % and 0.92 % for transverse electric and magnetic polarization, respectively, are present when the averaging area shape changes. According to the studied exposure scenarios, the area-averaged absorbed power density variations as a function of the averaging surface geometry are less significant than those related to the polarization of the incident field.
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