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在心肌细胞培养物中对强电休克诱发的心律失常进行光学映射。

Optical mapping of arrhythmias induced by strong electrical shocks in myocyte cultures.

作者信息

Fast Vladimir G, Cheek Eric R

机构信息

Department of Biomedical Engineering, University of Alabama at Birmingham, Birmingham, Al, USA.

出版信息

Circ Res. 2002 Apr 5;90(6):664-70. doi: 10.1161/01.res.0000013403.24495.cc.

DOI:10.1161/01.res.0000013403.24495.cc
PMID:11934833
Abstract

Strong electrical shocks can induce arrhythmias, which might explain why shocks fail to defibrillate. In this work, the localization of arrhythmia source and the relationship with local changes of transmembrane potential (V(m)) were determined in geometrically defined cell cultures using optical mapping technique. Uniform-field shocks with strength (E) of 10 to 50 V/cm were applied across cell strands with width of 0.2 and 0.8 mm. The threshold for arrhythmia induction was dependent on the strand width: in the 0.8- and 0.2-mm strands, arrhythmias were induced at E>/=20.6+/-1.8 V/cm (n=8) and E>/=30.3+/-1.8 V/cm (n=8), respectively. At the same shock strength, the arrhythmia rate and duration were larger in the wider strands. During shocks that induced arrhythmias, the V(m) waveforms on the anodal side revealed a positive V(m) shift that followed the initial large hyperpolarization and postshock elevation of the diastolic V(m). These V(m) changes were absent during failed shocks. To determine the localization of the arrhythmia source, arrhythmias were induced in narrow cell strands containing regions of local expansion. Optical mapping of the first extrabeat with a coupling interval of 315+/-60 ms revealed that in the majority of cases (9 out of 13) the source of arrhythmias was localized in the areas of shock-induced hyperpolarization. Thus, (1) induction of postshock arrhythmias, their rate, and their duration strongly depend on the tissue structure; (2) arrhythmia induction coincides with the appearance of a positive V(m) shift in the areas of hyperpolarization; and (3) the source of postshock arrhythmias is located in the areas of shock-induced hyperpolarization.

摘要

强电击可诱发心律失常,这或许能解释电击除颤为何失败。在本研究中,利用光学标测技术在几何形状明确的细胞培养物中确定心律失常源的定位及其与跨膜电位(V(m))局部变化的关系。对宽度为0.2毫米和0.8毫米的细胞束施加强度(E)为10至50伏/厘米的均匀电场电击。心律失常诱发阈值取决于细胞束宽度:在0.8毫米和0.2毫米的细胞束中,分别在E≥20.6±1.8伏/厘米(n = 8)和E≥30.3±1.8伏/厘米(n = 8)时诱发心律失常。在相同电击强度下,较宽细胞束中的心律失常发生率和持续时间更大。在诱发心律失常的电击过程中,阳极侧的V(m)波形显示出正的V(m)偏移,该偏移跟随初始的大幅超极化以及电击后舒张期V(m)的升高。在电击失败时不存在这些V(m)变化。为了确定心律失常源的定位,在包含局部扩张区域的狭窄细胞束中诱发心律失常。对耦合间期为(315±60)毫秒的第一个早搏进行光学标测显示,在大多数情况下(13例中的9例),心律失常源位于电击诱发超极化的区域。因此,(1)电击后心律失常的诱发、其发生率和持续时间强烈依赖于组织结构;(2)心律失常的诱发与超极化区域中V(m)正偏移的出现一致;(3)电击后心律失常的源位于电击诱发超极化的区域。

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