Reutskiy S, Rossoni E, Tirozzi B
Magnetohydrodynamics Laboratory, Moskovski Avenue 199, P.O. Box 136, 61037 Kharkov, Ukraine.
Biol Cybern. 2003 Dec;89(6):439-48. doi: 10.1007/s00422-003-0430-x. Epub 2003 Dec 4.
This study presents a model of action potential propagation in bundles of myelinated nerve fibers. The model combines the single-cable formulation of Goldman and Albus (1967) with a basic representation of the ephaptic interaction among the fibers. We analyze first the behavior of the conduction velocity (CV) under the change of the various conductance parameters and temperature. The main parameter influencing the CV is the fast sodium conductance, and the dependence of CV on the temperature is linear up to 30 degrees C. The increase of myelin thickness above its normal value (5 microm) gives a slight increase in CV. The CV of the single fiber decreases monotonically with the disruption of myelin, but the breakdown is abrupt. There is always conduction until the thickness is larger than 2% of its original value, at which with at this point a sharp transition of CV to zero occurs. Also, the increase of temperature can block conduction. At 5% of the original thickness there is still spike propagation, but an increase of 2 degrees C causes conduction block. These results are consistent with clinical observations. Computer simulations are performed to show how the CV is affected by local damage to the myelin sheath, temperature alterations, and increased ephaptic coupling (i.e., coupling of electrical origin due to the electric neutrality of all the nerve) in the case of fiber bundles. The ephaptic interaction is included in the model. Synchronous impulse transmission and the formation of "condensed" pulse states are found. Electric impulses with a delay of 0.5 ms are presented to the system, and the numerical results show that, for increasing coupling, the impulses tend to adjust their speed and become synchronized. Other interesting phenomena are that spurious spikes are likely to be generated when ephaptic interaction is raised and that damaged axons suffering conduction block can be brought into conduction by the normal functioning fibers surrounding them. This is seen also in the case of a large number of fibers (N=500). When all the fibers are stimulated simultaneously, the conduction velocity is found to be strongly dependent on the level of ephaptic coupling and a sensible reduction is observed with respect to the propagation along an isolated axon even for low coupling level. As in the case of three fibers, spikes tend to lock and form collective impulses that propagate slowly in the nerve. On the other hand, if only 10% of fibers are stimulated by an external input, the conduction velocity is only 2% less than that along a single axon. We found a threshold value for the ephaptic coupling such that for lower values it is impossible to recruit the damaged fibers into conduction, for values of the coupling equal to this threshold only one fiber can be restored by the nondamaged fibers, and for values larger than the threshold an increasing number of fibers can return to normal functioning. We get values of the ephaptic coupling such that 25% of axons can be damaged without change of the collective conduction.
本研究提出了一种有髓神经纤维束中动作电位传播的模型。该模型将戈德曼和阿尔布斯(1967年)的单电缆公式与纤维间电突触相互作用的基本表示相结合。我们首先分析了各种电导参数和温度变化下传导速度(CV)的行为。影响CV的主要参数是快速钠电导,在30摄氏度以下,CV对温度的依赖性是线性的。髓鞘厚度超过其正常值(5微米)会使CV略有增加。单根纤维的CV随着髓鞘的破坏而单调下降,但这种破坏是突然的。在厚度大于其原始值的2%之前总是存在传导,此时CV会急剧转变为零。此外,温度升高会阻断传导。在原始厚度的5%时仍有尖峰传播,但温度升高2摄氏度会导致传导阻断。这些结果与临床观察结果一致。进行了计算机模拟,以展示在纤维束的情况下,CV如何受到髓鞘局部损伤、温度变化和增强的电突触耦合(即由于所有神经的电中性而产生的电起源耦合)的影响。该模型包含了电突触相互作用。发现了同步冲动传递和“凝聚”脉冲状态的形成。向系统施加延迟为0.5毫秒的电冲动,数值结果表明,随着耦合增加,冲动倾向于调整其速度并变得同步。其他有趣的现象是,当电突触相互作用增强时可能会产生虚假尖峰,并且遭受传导阻断的受损轴突可以被周围正常功能的纤维带入传导状态。在大量纤维(N = 500)的情况下也观察到了这一点。当同时刺激所有纤维时,发现传导速度强烈依赖于电突触耦合水平,并且即使在低耦合水平下,相对于沿孤立轴突的传播也观察到了明显的降低。与三根纤维的情况一样,尖峰倾向于锁定并形成在神经中缓慢传播的集体冲动。另一方面,如果只有10%的纤维受到外部输入的刺激,传导速度仅比沿单根轴突的速度低2%。我们发现了电突触耦合的一个阈值,使得对于较低的值,不可能将受损纤维纳入传导,对于等于该阈值的耦合值,只有一根纤维可以被未受损纤维恢复传导,而对于大于该阈值的值,越来越多的纤维可以恢复正常功能。我们得到了电突触耦合的值,使得25%的轴突受损时集体传导不变。