A point source model to represent heat distribution without calculating the Joule heat during radiofrequency ablation

P. Mariappan, Gangadhara B , Ronan Flanagan 
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Abstract

Numerous liver cancer oncologists suggest bridging therapies to limit cancer growth until donors are available. Interventional radiology including radiofrequency ablation (RFA) is one such bridging therapy. This locoregional therapy aims to produce an optimal amount of heat to kill cancer cells, where the heat is produced by a radiofrequency (RF) needle. Less experienced Interventional Radiologists (IRs) require a software-assisted smart solution to predict the optimal heat distribution as both overkilling and untreated cancer cells are problematic treatments. Therefore, two of the big three partial differential equations, 1) heat equation (Pennes, Journal of Applied Physiology, 1948, 1, 93–122) to predict the heat distribution and 2) Laplace equation (Prakash, Open Biomed. Eng. J., 2010, 4, 27–38) for electric potential along with different cell death models (O’Neill et al., Ann. Biomed. Eng., 2011, 39, 570–579) are widely used in the last three decades. However, solving two differential equations and a cell death model is computationally expensive when the number of finite compact coverings of a liver topological structure increases in millions. Since the heat source from the Joule losses Q r = σ|∇V|2 is obtained from Laplace equation σΔV = 0, it is called the Joule heat model. The traditional Joule heat model can be replaced by a point source model to obtain the heat source term. The idea behind this model is to solve σΔV = δ 0 where δ 0 is a Dirac-delta function. Therefore, using the fundamental solution of the Laplace equation (Evans, Partial Differential Equations, 2010) we represent the solution of the Joule heat model using an alternative model called the point source model which is given by the Gaussian distribution. Q r x = ∑ x i ∈ Ω 1 K ∑ i c i e − | x − x i | 2 2 σ 2 where K and c i are obtained by using needle parameters. This model is employed in one of our software solutions called RFA Guardian (Voglreiter et al., Sci. Rep., 2018, 8, 787) which predicted the treatment outcome very well for more than 100 patients.
一个点源模型,以表示热分布不计算焦耳热在射频烧蚀
许多癌症肿瘤学家建议桥接疗法来限制癌症的生长,直到捐赠者可用。包括射频消融(RFA)在内的介入放射学就是这样一种桥接疗法。这种局部治疗旨在产生最佳的热量来杀死癌症细胞,其中热量是由射频(RF)针产生的。经验不足的介入放射科医生(IRs)需要软件辅助的智能解决方案来预测最佳热分布,因为过度杀伤和未经治疗的癌症细胞都是有问题的治疗方法。因此,三大偏微分方程中的两个,1)预测热分布的热方程(Pennes,Journal of Applied Physiology,1948,193-122)和2)电势的拉普拉斯方程(Prakash,Open Biomed.Eng.J.,2010,4,27-38)以及不同的细胞死亡模型(O'Neill et al.,Ann。生物识别。Eng.,2011,39570–579)在过去三十年中被广泛使用。然而,当肝脏拓扑结构的有限紧致覆盖物的数量以百万计增加时,求解两个微分方程和细胞死亡模型的计算成本很高。由于焦耳损失的热源Q r=σ|ŞV|2是由拉普拉斯方程σΔV=0得到的,因此称为焦耳热模型。可以用点源模型代替传统的焦耳热模型来获得热源项。该模型背后的思想是求解σΔV=δ0,其中δ0是狄拉克德尔塔函数。因此,使用拉普拉斯方程的基本解(Evans,偏微分方程,2010),我们使用称为点源模型的替代模型来表示焦耳热模型的解,该模型由高斯分布给出。Q r x=∑x i∈Ω1 K∑i c i e−| x−x i |2 2σ2其中K和c i是通过使用针状参数获得的。该模型被用于我们的一个名为RFA Guardian的软件解决方案(Voglreiter等人,Sci.Rep.,2018,8787),该解决方案很好地预测了100多名患者的治疗结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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