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Clini-Therm施药器在非均匀平面组织模型上的时域有限差分模拟。

FDTD simulations of Clini-Therm applicators on inhomogeneous planar tissue models.

作者信息

Chan K W, McDougall J A, Chou C K

机构信息

City of Hope National Medical Center, Duarte, CA 91010-3000, USA.

出版信息

Int J Hyperthermia. 1995 Nov-Dec;11(6):809-20. doi: 10.3109/02656739509052337.

DOI:10.3109/02656739509052337
PMID:8586902
Abstract

A finite-difference time-domain (FDTD) algorithm was used to compute SAR distributions in planar fat-muscle phantom exposed to the Clini-Therm microwave applicators. The models consisted of a 30 X 30 X 7.5 cm phantom and a 15 X 15 cm, 10 X 10 cm or 7.5 X 7.5 cm aperture dielectric slab loaded applicator. The phantom was either filled with muscle material or with 1.0 cm fat on 6.5 cm muscle. A mineral oil bolus was placed on the fat-muscle model with its integrated water channels parallel to the electric or magnetic field. The FDTD resolution was 3 mm and the applicators were excited with a Gaussian pulse. The computations required 6000-8000 time steps to reach steady state, with 45-48 Mwords on a Cray Y-MP C-90 in 1000-1200 CPU seconds. The electric field components at 915 MHz were obtained by summing the Fourier coefficients at each grid point during each time step and SAR was determined. The results were qualitatively compared to existing and published thermographic heating patterns with good agreement. The computed electric field distributions had provided a three dimensional view into the problem space to investigate and understand wave propagation phenomena in complex inhomogeneous configurations that were not feasible with experimental models.

摘要

采用时域有限差分(FDTD)算法计算了暴露于Clini-Therm微波辐射器的平面脂肪-肌肉模型中的比吸收率(SAR)分布。模型包括一个30×30×7.5厘米的模型以及一个15×15厘米、10×10厘米或7.5×7.5厘米孔径的加载介质板辐射器。模型中要么填充肌肉材料,要么在6.5厘米厚的肌肉上覆盖1.0厘米厚的脂肪。在脂肪-肌肉模型上放置了一个矿物油推注器,其集成水通道与电场或磁场平行。FDTD分辨率为3毫米,辐射器由高斯脉冲激发。计算需要6000 - 8000个时间步长才能达到稳态,在Cray Y-MP C-90上运行1000 - 1200个CPU秒,占用45 - 48兆字的内存。通过在每个时间步长对每个网格点的傅里叶系数求和获得915 MHz时的电场分量,并确定SAR。将结果与现有的和已发表的热成像加热模式进行定性比较,结果吻合良好。计算得到的电场分布提供了问题空间的三维视图,以研究和理解复杂非均匀结构中的波传播现象,这对于实验模型来说是不可行的。

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