a BioMIT-Department of Electronic Engineering , Universitat Politècnica de València , Valencia , Spain.
Int J Hyperthermia. 2018 May;34(3):243-249. doi: 10.1080/02656736.2017.1336258. Epub 2017 Jun 18.
The thermal effect of the intramyocardial blood perfusion on the size of lesions created by radiofrequency cardiac ablation (RFCA) has not been adequately studied to date. Our objective was to assess the impact of including this phenomenon in RFCA computer modelling in terms of the thermal lesion depth created.
A computer model was built and computer simulations were conducted to assess the effect of including the blood perfusion term in the bioheat equation. This term mimics the intramyocardial blood flow (i.e., blood perfusion) in the cardiac wall at the site at which the RFCA is being conducted and hence represents a heat removing mechanism. When considered, blood perfusion rates ranged from 609 to 1719 ml/min/kg. Two electrode design and modes were considered: a non-irrigated electrode with constant temperature mode and an irrigated electrode with constant power mode.
All the depths computed without including the blood perfusion term were larger than those that did include it, regardless of perfusion rate. The differences in lesion depth between ignoring and including blood perfusion increased over time; for a 60 s RFCA they were 0.45 and 1 mm for minimum and maximum perfusion rate, respectively. The differences were more or less independent of blood flow in the cardiac chamber, electrode type and ablation mode.
The findings suggest that the heat-sink effect of blood perfusion should be taken into account in the case of ablations (>1 minute) such as those conducted in RFCA of the ventricular wall.
目前,关于心肌内血液灌注对射频心脏消融(RFCA)所产生的病变大小的热效应尚未进行充分研究。我们的目的是评估在 RFCA 计算机建模中考虑这一现象对产生的热损伤深度的影响。
建立了一个计算机模型,并进行了计算机模拟,以评估在生物热方程中包含血液灌注项的效果。该术语模拟了在进行 RFCA 的心脏壁部位的心肌内血流(即血液灌注),因此代表了一种热量去除机制。当考虑时,血液灌注率范围为 609 至 1719 ml/min/kg。考虑了两种电极设计和模式:带恒温水温模式的非灌流电极和带恒功率模式的灌流电极。
无论灌注率如何,所有未包含血液灌注项计算的损伤深度都大于包含该项的损伤深度。忽略和包含血液灌注之间的损伤深度差异随时间增加;对于 60 秒的 RFCA,最小和最大灌注率分别为 0.45 和 1 毫米。这些差异或多或少独立于心脏腔室中的血流、电极类型和消融模式。
研究结果表明,在消融(>1 分钟)的情况下,如在心室壁的 RFCA 中,应考虑血液灌注的热阱效应。