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沿分支轴突传导动作电位的数学模型。

A mathematical model for conduction of action potentials along bifurcating axons.

作者信息

Parnas I, Segev I

出版信息

J Physiol. 1979 Oct;295:323-43. doi: 10.1113/jphysiol.1979.sp012971.

Abstract
  1. A mathematical model based on the Hodgkin-Huxley equations is derived to describe quantitatively the propagation of action potentials in a branching axon. 2. The model treats the case of a bifurcating axon with branches of different diameters. The solution takes into account the changes in space constant in the different regions. 3. The model allows for investigating parameters leading to preferential conduction of action potentials in one daughter branch as seen experimentally. 4. Assuming that the only difference between the various daughter branches is in their diameters, conduction blocks should occur simultaneously rather than differentially into all daughter branches when the geometrical ratio is greater than 10. 5. In order to obtain differential conduction into the two branches changes in ionic concentrations due to the repetitive action potentials had to be introduced into the equations. 6. We find that conditions which allow differential buildup of K concentration around the two branches, produce differential conduction block. These conditions may be different periaxonal spaces around the branches or different time constant for recovery processes that eliminate K from the periaxonal space. 7. The effects of an inexcitable branch on conduction of action potentials in the second branch are described. 8. We find that the membrane current which is associated with the action potential is much more sensitive than the action potential itself and shows more distinct changes near regions of inhomogeneity such as a branch point, a step increase in diameter or an inexcitable branch.
摘要
  1. 基于霍奇金-赫胥黎方程推导了一个数学模型,用于定量描述动作电位在分支轴突中的传播。2. 该模型处理具有不同直径分支的分叉轴突的情况。该解考虑了不同区域空间常数的变化。3. 该模型允许研究导致动作电位在一个子分支中优先传导的参数,正如实验中所观察到的那样。4. 假设各个子分支之间的唯一差异在于它们的直径,当几何比率大于10时,传导阻滞应同时发生,而不是差异地发生在所有子分支中。5. 为了在两个分支中获得差异传导,必须将由于重复动作电位引起的离子浓度变化引入方程中。6. 我们发现,允许在两个分支周围差异积累钾离子浓度的条件会产生差异传导阻滞。这些条件可能是分支周围不同的轴周间隙,或者是从轴周间隙消除钾离子的恢复过程的不同时间常数。7. 描述了一个不可兴奋分支对第二个分支中动作电位传导的影响。8. 我们发现,与动作电位相关的膜电流比动作电位本身更敏感,并且在不均匀区域(如分支点、直径阶跃增加或不可兴奋分支)附近表现出更明显的变化。

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