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浦肯野纤维缝隙中钾离子蓄积的模拟:对膜电活动的影响。

Simulation of potassium accumulation in clefts of Purkinje fibers: effect on membrane electrical activity.

作者信息

Coulombe A, Coraboeuf E

出版信息

J Theor Biol. 1983 Sep 21;104(2):211-29. doi: 10.1016/0022-5193(83)90411-3.

Abstract

Purkinje fiber action potentials and concomitant intercellular cleft [K] variations were reconstructed by using modified McAllister, Noble & Tsien (1975) equations including the pump current, ip, and the pacemaker current, if. Three different mean cleft widths were chosen: 40, 200 and 1000 nm. Assuming a cylindrical arrangement of the cells in the bundle, the cleft [K] gradient across the bundle was calculated by using the radial cylindrical diffusion equation. The effects of varying several parameters (cleft width, tortuosity, ip and if) were studied in conditions corresponding to two different values of [K] in the bulk solution, namely 2.7 and 5.4 mM. The shortening influence on the action potential of the systolic increase in cleft [K] was detectable only in the case of the smallest cleft width. Reduction in electrogenic pump activity led to alterations of the electrical activity which depended on the cleft width. The evolution of the intercellular [K] during each action potential and the following diastolic period was normally biphasic; a small reaccumulation during the late part of the diastole was induced by the K component of the if current. Experimentally determined intercellular [K] variations described in the literature exhibit a monophasic evolution. Such a monophasic evolution could be reproduced after reduction of both if and the transient outward K current and suppression of the negative slope of the ik1-Em relationship. In this case the amplitude of the cyclic change in intercellular [K] was approximately equal to 0.2 mM (for a 200 nm cleft width), a value much lower than that experimentally recorded. Possible reasons for this discrepancy are discussed. A simplified three compartment model for K diffusion was also used. Results obtained with the two models demonstrated that the simplified model can be used as a reasonable approximation of the more complex radial diffusion model, with a reduction in computation time reaching 80% or more.

摘要

通过使用修正的麦卡利斯特、诺布尔和钱(1975年)方程,包括泵电流(i_p)和起搏电流(i_f),重建了浦肯野纤维动作电位和伴随的细胞间裂隙[K]变化。选择了三种不同的平均裂隙宽度:40、200和1000纳米。假设束中细胞呈圆柱形排列,使用径向圆柱扩散方程计算束中裂隙[K]梯度。在对应于本体溶液中两种不同[K]值(即2.7和5.4毫摩尔)的条件下,研究了改变几个参数(裂隙宽度、曲折度、(i_p)和(i_f))的影响。仅在最小裂隙宽度的情况下,才能检测到收缩期裂隙[K]增加对动作电位的缩短影响。电生泵活性降低导致电活动改变,这取决于裂隙宽度。每个动作电位和随后舒张期细胞间[K]的演变通常是双相的;舒张后期的小再积累是由(i_f)电流的K成分诱导的。文献中描述的实验测定的细胞间[K]变化呈现单相演变。在降低(i_f)和瞬时外向K电流并抑制(i_{K1}-E_m)关系的负斜率后,可以再现这种单相演变。在这种情况下,细胞间[K]循环变化的幅度约为0.2毫摩尔(对于200纳米的裂隙宽度),该值远低于实验记录的值。讨论了这种差异的可能原因。还使用了一个简化的三室K扩散模型。用这两个模型得到的结果表明,简化模型可以用作更复杂的径向扩散模型的合理近似,计算时间减少达80%或更多。

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