Kerckhoffs Roy C P, Faris Owen P, Bovendeerd Peter H M, Prinzen Frits W, Smits Karel, McVeigh Elliot R, Arts Theo
Department of Biomedical Engineering, Eindhoven University of Technology, Eindhoven, The Netherlands.
J Cardiovasc Electrophysiol. 2003 Oct;14(10 Suppl):S188-95. doi: 10.1046/j.1540.8167.90310.x.
For efficient pump function, contraction of the heart should be as synchronous as possible. Ventricular pacing induces asynchrony of depolarization and contraction. The degree of asynchrony depends on the position of the pacing electrode. The aim of this study was to extend an existing numerical model of electromechanics in the left ventricle (LV) to the application of ventricular pacing. With the model, the relation between pacing site and patterns of depolarization and contraction was investigated.
The LV was approximated by a thick-walled ellipsoid with a realistic myofiber orientation. Propagation of the depolarization wave was described by the eikonal-diffusion equation, in which five parameters play a role: myocardial and subendocardial velocity of wave propagation along the myofiber cm and ce; myocardial and subendocardial anisotropy am and ae; and parameter k, describing the influence of wave curvature on wave velocity. Parameters cm, ae, and k were taken from literature. Parameters am and ce were estimated by fitting the model to experimental data, obtained by pacing the canine left ventricular free wall (LVFW). The best fit was found with cm = 0.75 m/s, ce = 1.3 m/s, am = 2.5, ae = 1.5, and k = 2.1 x 10(-4) m2/s. With these parameter settings, for right ventricular apex (RVA) pacing, the depolarization times were realistically simulated as also shown by the wavefronts and the time needed to activate the LVFW. The moment of depolarization was used to initiate myofiber contraction in a model of LV mechanics. For both pacing situations, mid-wall circumferential strains and onset of myofiber shortening were obtained.
With a relatively simple model setup, simulated depolarization timing patterns agreed with measurements for pacing at the LVFW and RVA in an LV. Myocardial cross-fiber wave velocity is estimated to be 0.40 times the velocity along the myofiber direction (0.75 m/s). Subendocardial wave velocity is about 1.7 times faster than in the rest of the myocardium, but about 3 times slower than as found in Purkinje fibers. Furthermore, model and experiment agreed in the following respects. (1) Ventricular pacing decreased both systolic pressure and ejection fraction relative to natural sinus rhythm. (2) In early depolarized regions, early shortening was observed in the isovolumic contraction phase; in late depolarized regions, myofibers were stretched in this phase. Maps showing timing of onset of shortening were similar to previously measured maps in which wave velocity of contraction appeared similar to that of depolarization.
为实现有效的泵功能,心脏收缩应尽可能同步。心室起搏会导致去极化和收缩的不同步。不同步程度取决于起搏电极的位置。本研究的目的是将现有的左心室机电数值模型扩展至心室起搏的应用。利用该模型,研究了起搏部位与去极化和收缩模式之间的关系。
左心室由具有实际肌纤维取向的厚壁椭球体近似表示。去极化波的传播由程函扩散方程描述,其中五个参数起作用:沿肌纤维的心肌和心内膜下波传播速度(cm)和(ce);心肌和心内膜下各向异性(am)和(ae);以及描述波曲率对波速影响的参数(k)。参数(cm)、(ae)和(k)取自文献。参数(am)和(ce)通过将模型拟合到通过对犬左心室游离壁(LVFW)起搏获得的实验数据来估计。发现最佳拟合参数为(cm = 0.75 m/s),(ce = 1.3 m/s),(am = 2.5),(ae = 1.5),(k = 2.1×10^{-4} m^2/s)。通过这些参数设置,对于右心室心尖(RVA)起搏,去极化时间得到了逼真的模拟,波前和激活LVFW所需的时间也表明了这一点。去极化时刻用于启动左心室力学模型中的肌纤维收缩。对于两种起搏情况,均获得了中层圆周应变和肌纤维缩短的起始情况。
通过相对简单的模型设置,模拟的去极化时间模式与左心室中LVFW和RVA起搏的测量结果一致。估计心肌跨纤维波速是沿肌纤维方向波速(0.75 m/s)的0.40倍。心内膜下波速比心肌其他部分快约1.7倍,但比浦肯野纤维中的波速慢约3倍。此外,模型与实验在以下方面一致。(1)与自然窦性心律相比,心室起搏降低了收缩压和射血分数。(2)在早期去极化区域,等容收缩期观察到早期缩短;在晚期去极化区域,此阶段肌纤维被拉伸。显示缩短起始时间的图谱与先前测量的图谱相似,其中收缩波速似乎与去极化波速相似。