Kogan B Y, Karplus W J, Billett B S, Pang A T, Khan S S, Mandel W J, Karagueuzian H S
Department of Computer Sciences, UCLA.
Pacing Clin Electrophysiol. 1991 Nov;14(11 Pt 2):1688-93. doi: 10.1111/j.1540-8159.1991.tb02749.x.
The mechanism of induced reentry in an initially homogeneous repolarization matrix still remains undefined. In the present study we hypothesized that the slow deactivation rate of the delayed outward current (dIo/dt), which occurs during diastole after complete repolarization, can cause activation failure and facilitate reentry. We modeled the excitation-recovery process using the modified FitzHugh-Nagumo equations in a two-dimensional medium of 128 by 128 cells using the Connection Machine (CM-2), a massively parallel computer that is highly suitable for this class of problem. The model was one cell thick, uniformly excitable, and isotropic. When the rate of Io deactivation was slowed to yield action potential duration (APD) restitution curves similar to experimentally observed arrhythmic ventricular muscle cells ADP restitution curves, premature stimulation (S2) induced nonstationary double spiral waves (Figure 8 reentry). A decrease in dIo/dt increased the radius of the circle around which the tip of the spiral waves rotates and decreased its angular velocity. Wave fronts propagated through areas where the residual diastolic Io was fully inactivated and blocked in areas where its amplitude was high. No such dynamics of wave front propagation could be induced when S2 was applied after the completion of Io deactivation. We conclude that the kinetics of deactivation of the Io during diastole has a profound influence on the dynamics of two-dimensional wave front propagation. The similarities of the APD restitution curve implemented in the computer model with slow deactivation of Io and that observed in our canine model of quinidine induced ventricular tachyarrhythmias suggest that Io deactivation kinetics may play an important role in arrhythmogenesis in the intact ventricle.
在初始均匀复极化基质中诱导折返的机制仍未明确。在本研究中,我们假设在完全复极化后的舒张期发生的延迟外向电流(dIo/dt)缓慢失活速率,可导致激活失败并促进折返。我们使用改良的FitzHugh-Nagumo方程,在由128×128个细胞组成的二维介质中,利用连接机(CM-2,一种非常适合此类问题的大规模并行计算机)对兴奋-恢复过程进行建模。该模型为单层细胞,具有均匀的兴奋性且各向同性。当Io失活速率减慢以产生与实验观察到的心律失常性心室肌细胞动作电位时程(APD)恢复曲线相似的APD恢复曲线时,过早刺激(S2)可诱导非平稳双螺旋波(图8折返)。dIo/dt的降低增加了螺旋波尖端围绕其旋转的圆的半径,并降低了其角速度。波前传播通过残余舒张期Io完全失活的区域,并在其幅度较高的区域受阻。当在Io失活完成后施加S2时,不会诱导出这种波前传播动力学。我们得出结论,舒张期Io的失活动力学对二维波前传播动力学有深远影响。计算机模型中Io缓慢失活时实现的APD恢复曲线与我们在奎尼丁诱导的犬室性心律失常模型中观察到的曲线相似,这表明Io失活动力学可能在完整心室的心律失常发生中起重要作用。