Taniguchi A, Toyama J, Kodama I, Anno T, Shirakawa M, Usui S
Department of Circulation, Nagoya University, Japan.
Am J Physiol. 1994 Aug;267(2 Pt 2):H694-705. doi: 10.1152/ajpheart.1994.267.2.H694.
To clarify the mechanism underlying the ectopic excitation after countershock, the cellular activation processes of cardiac tissue with a low-potential-gradient electric field (LPEF) were investigated in experiments using guinea pig papillary muscles and in computer simulation. Action potential upstrokes in papillary muscles during longitudinal propagation (LP) or transverse propagation (TP) were different from those of nonpropagating ones in single ventricular cells in terms of lower maximum upstroke velocity (Vmax) (LP, 231 V/s; TP, 309 V/s) and the presence of a linear ascending segment in the phase-plane plot. High Vmax (409 V/s) close to the single cell (512 V/s) was obtained in the muscle at the collision of LP (LC). Field stimulation of the muscles with LPEF < 5 V/cm caused inhomogeneous excitation suggesting multiple wave fronts, which collide with each other, and a wide spatial dispersion of Vmax (132-388 V/s). Phase-plane plots of action potential with lower Vmax were similar to LP or TP, whereas those with higher Vmax were similar to LC. In the two-dimensional discrete sheet composed of 51 x 51 elements of modified Beeler-Reuter model, the inhomogeneous excitation induced by LPEF is mimicked by setting a random variation of stimulus onset in each element. LPEF may induce inhomogeneous excitation with multiple wave fronts through a complex electrotonic interaction. This would provide a basis for the genesis of ectopic focal excitation.
为阐明电击后异位兴奋的潜在机制,在豚鼠乳头肌实验和计算机模拟中研究了低电位梯度电场(LPEF)作用下心脏组织的细胞激活过程。在纵向传播(LP)或横向传播(TP)过程中,乳头肌动作电位的上升支与单个心室细胞中不传播的动作电位上升支不同,表现为最大上升速度(Vmax)较低(LP为231V/s;TP为309V/s),且相平面图中存在线性上升段。在LP碰撞(LC)时,肌肉中获得了接近单细胞(512V/s)的高Vmax(409V/s)。用<5V/cm的LPEF对肌肉进行电场刺激会导致不均匀兴奋,提示存在多个相互碰撞的波前,且Vmax存在广泛的空间离散(132 - 388V/s)。Vmax较低的动作电位相平面图与LP或TP相似,而Vmax较高的相平面图与LC相似。在由51×51个修改后的Beeler - Reuter模型元素组成的二维离散薄片中,通过在每个元素中设置刺激起始的随机变化来模拟LPEF诱导的不均匀兴奋。LPEF可能通过复杂的电紧张相互作用诱导具有多个波前的不均匀兴奋。这将为异位灶性兴奋的发生提供基础。