从分析和数值模拟深入了解心内电图

L. Leenknegt, K. Zeppenfeld, A. Panfilov, H. Dierckx
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引用次数: 0

摘要

经费来源类型:基金会。心脏电图(EGMs)是电解剖电压测绘过程中获得的最重要的记录之一,是规划大多数临床电生理干预措施的基础。尽管它被广泛使用,但EGM的形状和振幅与心脏组织的潜在兴奋模式和特性的关系尚未完全了解。最近的临床研究为EGM振幅与心肌壁厚度之间的关系提供了重要的新指导。本研究的目的是利用分析和计算机方法量化壁厚对EGM振幅和持续时间的影响。我们在心脏组织的均匀板(70 x 70 x L mm)中进行了双极EGMs的硅质和解析性研究,其中L = 2、5或10 mm,具有平行纤维方向。使用心脏电生理模拟器openCARP[2]进行模拟。用10只Tusscher-Panfilov 2006模型(TP06)[4]描述心肌细胞,并记录心外膜组织参数。产生沿光纤方向传播的平面波。为了研究双极电极取向对细胞外电压的影响(见图1A[3]),我们测量了围绕一个点呈半球排列的147个点的细胞外电压。此外,我们开发了一种解析方法来获得EGM,使用去极化波前的等效偶极子表示和相应积分的解析计算。图1B和1C显示了EGM性能与电极方向的关系,用α(入射角)和β(电极与传播方向之间的夹角)[3]表示。实线表示最先进的数值方法的数据,虚线表示我们的分析估计。我们的理论可以很好地近似于电极所有方向的峰间振幅和EGM宽度。图2显示了心肌壁厚l对EGM的影响,其振幅和持续时间都与我们的理论很好地吻合。我们观察到振幅和宽度随着板坯厚度的增加而增加,证实了[1]的结果,但也为这种变化提供了准确的分析表达式。因此,它可以区分厚度和影响egm的其他因素的影响,例如衬底异常。我们开发了一种能够正确描述EGM去极化部分的振幅、持续时间和形状的分析方法。我们的理论与之前关于导管定向[3,5]和管壁厚度[1,3]影响的计算机和临床研究一致。该方向的后续工作有望为egm的临床解释提供更好的指导,考虑心肌壁厚度在心律失常底物表征中的作用。
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Insights into the intracardiac electrogram from analytical and numerical modelling
Type of funding sources: Foundation. Main funding source(s): FWO-Flanders, KU Leuven internal starting grant Cardiac electrograms (EGMs) are one of the most important recordings obtained during electroanatomical voltage mapping and lie at the basis for planning most clinical electrophysiological interventions. Despite its widespread use, the relation of EGM shape and amplitude to the underlying excitation patterns and properties of cardiac tissue is not completely understood. Recent clinical studies [1] have provided important new guidelines on the relation between EGM amplitudes and the thickness of myocardial walls. The aim of this study is to quantify the effect of the wall thickness on EGM amplitudes and duration using analytical and in-silico approaches. We study bipolar EGMs both in-silico and analytically in a homogeneous slab of cardiac tissue (70 x 70 x L mm), where L = 2, 5, or 10 mm, with parallel fiber direction. Simulations were performed using the cardiac electrophysiology simulator openCARP [2]. Cardiac cells were described by the ten Tusscher-Panfilov 2006 model (TP06) [4] with epicardial tissue parameters. A plane wave propagating along the fiber direction was initiated. The extracellular voltage at 147 points arranged in a hemisphere around a point was measured to study the effect of bipolar electrode orientation (see Fig. 1A [3]). In addition, we developed an analytical approach to obtain an EGM, using an equivalent dipole representation of the depolarization wavefront and analytical evaluation of the corresponding integrals. Fig. 1B and 1C show the dependency of the EGM properties on the electrode orientation, as represented by the angles α (incidence angle) and β (angle between electrode and propagation direction) [3]. Solid lines represent data from a state-of-the-art numerical methodology, the dashed lines show our analytical estimations. Both the peak-to-peak amplitude and EGM width are well approximated by our theory for all orientations of the electrodes. Fig. 2 shows how the EGM is influenced by the myocardial wall thickness L. Both the amplitude and the duration are in good agreement with our theory. We observe that the amplitude as well as the width increase with the slab thickness, confirming the result in [1] but also delivering an accurate analytical expression for this change. It may thus allow to discriminate effects of thickness and other factors affecting the EGMs, such as substrate abnormalities, for example. We developed an analytical approach which can correctly describe the amplitude, duration, and shape of the depolarization part of the EGM. Our theory agrees with the previous in-silico and clinical studies on the influence of catheter orientation [3,5], and wall thickness [1,3]. Subsequent work in this direction is expected to provide better guidelines for clinical interpretation of EGMs, accounting for the effects of the thickness of myocardial wall in the characterization of the substrate of cardiac arrhythmias.
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