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哺乳动物有髓轴突动作电位和后电位的计算机模拟:低电阻髓鞘的情况

Computer simulation of action potentials and afterpotentials in mammalian myelinated axons: the case for a lower resistance myelin sheath.

作者信息

Blight A R

出版信息

Neuroscience. 1985 May;15(1):13-31. doi: 10.1016/0306-4522(85)90119-8.

Abstract

Depolarizing afterpotentials, recorded in peripheral nerves [Barrett and Barrett (1982) J. Physiol., Lond. 323, 117-144] and spinal axons [Blight and Someya (1985) Neuroscience 15, 1-12], have been interpreted as representing passive discharge of axolemmal capacitance. This interpretation requires a lower resistance pathway through the myelin sheath than previous measurements have suggested. A computer model was used to examine the contribution of the electrical characteristics of nerve fibers to action potential conduction and afterpotential generation. The model consisted of a resistance-capacitance network representing a chain of 20 internodes. The resistances of node, internode and myelin sheath, deduced from observations in the accompanying paper, [Blight and Someya (1985) Neuroscience, 15] were found to produce suitable length and time constants, and prolonged afterpotentials, when inserted into the model. Similar length and time constants were found using a conventional model of the axon, based on measurements from isolated peripheral fibers, but this did not reproduce the afterpotentials. Action-potential conduction velocity is enhanced by reducing the time constant and increasing the length constant. The problem of minimizing the internodal time constant was met in the conventional model through the low parallel resistance of the node, while in the new model it was met by reducing the resistance of the myelin sheath. The latter strategy required the nodal leakage resistance to be higher than values from single fiber measurements (ca 250 M omega rather than ca 50 M omega) in order to maintain the length constant similar to the conventional model. Simulation of the recorded potentials required the resistance of the myelin lamellae to be approx. 100 omega cm2. The model quantitatively reproduced the voltage response of the axon to injected current pulses and to propagated action potentials, using Frankenhaeuser-Huxley kinetics. [Frankenhaeuser and Huxley (1964) J. Physiol., Lond. 171, 302-315; Frankenhaeuser and Moore (1963) J. Physiol., Lond. 169, 431-437]. The short duration components of the afterpotential, observed in mammalian recordings were reproduced by assuming a leakage pathway in the myelin sheath, at the impalement site. The calculated lower resistance of the myelin sheath was such that it minimized the effective internodal time constant for a given nodal resistance. This appears to free the myelinated fiber from the alternative requirement for a high nodal leakage conductance.(ABSTRACT TRUNCATED AT 400 WORDS)

摘要

在周围神经[巴雷特和巴雷特(1982年),《伦敦生理学杂志》323卷,117 - 144页]和脊髓轴突[布莱特和染谷(1985年),《神经科学》15卷,1 - 12页]中记录到的去极化后电位,被解释为轴膜电容的被动放电。这种解释要求髓鞘中有一条电阻比先前测量结果所显示的更低的通路。使用一个计算机模型来研究神经纤维的电学特性对动作电位传导和后电位产生的贡献。该模型由一个电阻 - 电容网络组成,代表20个节间的链。从随附论文[布莱特和染谷(1985年),《神经科学》15卷]中的观察结果推导得出的节点、节间和髓鞘的电阻,当插入模型时,被发现能产生合适的长度和时间常数以及延长的后电位。基于对分离的周围纤维的测量,使用传统的轴突模型也发现了类似的长度和时间常数,但这并没有重现后电位。通过减小时间常数和增加长度常数可以提高动作电位的传导速度。在传统模型中,通过节点的低并联电阻解决了最小化节间时间常数的问题,而在新模型中则通过降低髓鞘的电阻来解决。后一种策略要求节点泄漏电阻高于单纤维测量值(约250兆欧而不是约50兆欧),以便维持与传统模型相似的长度常数。对记录电位的模拟要求髓鞘薄片的电阻约为100欧·平方厘米。该模型使用弗兰肯海默 - 赫胥黎动力学定量地重现了轴突对注入电流脉冲和传播动作电位的电压响应。[弗兰肯海默和赫胥黎(1964年),《伦敦生理学杂志》171卷,302 - 315页;弗兰肯海默和摩尔(1963年),《伦敦生理学杂志》169卷,431 - 437页]。在哺乳动物记录中观察到的后电位的短持续时间成分,通过假设在刺入部位的髓鞘中有一条泄漏通路得以重现。计算得出的髓鞘较低电阻使得在给定的节点电阻下,有效节间时间常数最小化。这似乎使有髓纤维摆脱了对高节点泄漏电导的另一种要求。(摘要截取自400字)

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