{"title":"Effect of anisotropy in myocardial electrical conductivity on lesion characteristics during radiofrequency cardiac ablation: a numerical study.","authors":"Kaihao Gu, Shengjie Yan, Xiaomei Wu","doi":"10.1080/02656736.2021.2022220","DOIUrl":null,"url":null,"abstract":"<p><strong>Background: </strong>Traditional computer simulation studies of radiofrequency catheter ablation (RFCA) usually neglect the anisotropy in myocardial electrical conductivity (MEC), which is likely an essential factor in governing the ablation outcome. Here, a numerical study of lesion characteristics during RFCA based on an anatomy-based model incorporating fiber orientation was performed to investigate the anisotropy in MEC.</p><p><strong>Methods: </strong>A three-dimensional thorax model including atria, blood, connective tissue, muscle, fat, and skin was constructed. The myocardial fiber was established through a rule-based method (RBM) based on the anatomical structure of the heart. The anisotropic MEC were 0.40 and 0.28 S m<sup>-1</sup> in longitudinal and transverse directions, respectively. The ablation result was compared with the isotropic scenario where the isotropic MEC was the average of the anisotropic conductivities as 0.34 S m<sup>-1</sup>.</p><p><strong>Results: </strong>The complexity of fiber architecture varied with that of the local anatomical structure. At RF power of 20 W for 30 s, the tissue temperature and lesion volume were reduced by 2.8 ± 0.1% and 6.9 ± 0.5%, respectively, under anisotropic MEC around the ostium of the pulmonary vein and left atrial appendage. Those for the posterior wall and roof of the left atrium, and the inside of the superior vena cava were 1.9 ± 0.3% and 5.6 ± 1.2%, respectively.</p><p><strong>Conclusions: </strong>Anisotropy in MEC has a greater reduction effect on lesion volume than on tissue temperature during RFCA; this effect tends to be restrained at positions with more uniform fiber distributions and can be enhanced where significant variation in fiber architecture occurred.</p>","PeriodicalId":520653,"journal":{"name":"International journal of hyperthermia : the official journal of European Society for Hyperthermic Oncology, North American Hyperthermia Group","volume":" ","pages":"120-133"},"PeriodicalIF":3.0000,"publicationDate":"2022-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International journal of hyperthermia : the official journal of European Society for Hyperthermic Oncology, North American Hyperthermia Group","FirstCategoryId":"3","ListUrlMain":"https://doi.org/10.1080/02656736.2021.2022220","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 4
Abstract
Background: Traditional computer simulation studies of radiofrequency catheter ablation (RFCA) usually neglect the anisotropy in myocardial electrical conductivity (MEC), which is likely an essential factor in governing the ablation outcome. Here, a numerical study of lesion characteristics during RFCA based on an anatomy-based model incorporating fiber orientation was performed to investigate the anisotropy in MEC.
Methods: A three-dimensional thorax model including atria, blood, connective tissue, muscle, fat, and skin was constructed. The myocardial fiber was established through a rule-based method (RBM) based on the anatomical structure of the heart. The anisotropic MEC were 0.40 and 0.28 S m-1 in longitudinal and transverse directions, respectively. The ablation result was compared with the isotropic scenario where the isotropic MEC was the average of the anisotropic conductivities as 0.34 S m-1.
Results: The complexity of fiber architecture varied with that of the local anatomical structure. At RF power of 20 W for 30 s, the tissue temperature and lesion volume were reduced by 2.8 ± 0.1% and 6.9 ± 0.5%, respectively, under anisotropic MEC around the ostium of the pulmonary vein and left atrial appendage. Those for the posterior wall and roof of the left atrium, and the inside of the superior vena cava were 1.9 ± 0.3% and 5.6 ± 1.2%, respectively.
Conclusions: Anisotropy in MEC has a greater reduction effect on lesion volume than on tissue temperature during RFCA; this effect tends to be restrained at positions with more uniform fiber distributions and can be enhanced where significant variation in fiber architecture occurred.
背景:传统的射频导管消融(RFCA)计算机模拟研究通常忽略了心肌电导率(MEC)的各向异性,而这可能是控制消融结果的重要因素。本文基于解剖学模型,结合纤维取向,对RFCA过程中的病变特征进行了数值研究,以研究MEC的各向异性。方法:建立包括心房、血液、结缔组织、肌肉、脂肪、皮肤在内的三维胸腔模型。基于心脏解剖结构,采用规则法(RBM)建立心肌纤维。各向异性MEC在纵向和横向分别为0.40和0.28 S m-1。将烧蚀结果与各向同性情况下各向同性MEC为各向异性电导率的平均值0.34 S m-1进行了比较。结果:纤维结构的复杂性随局部解剖结构的不同而不同。射频功率为20 W,持续30 s,各向异性MEC下肺静脉口周围组织温度和病变体积分别降低2.8±0.1%和6.9±0.5%。左心房后壁、顶部和上腔静脉内侧分别为1.9±0.3%和5.6±1.2%。结论:在RFCA过程中,MEC各向异性对病变体积的减小作用大于对组织温度的减小作用;这种效应往往在纤维分布更均匀的位置受到抑制,在纤维结构发生显著变化的地方可以增强。