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霍奇金-赫胥黎方程的孤立周期解。

Isolated periodic solutions of the Hodgkin-Huxley equations.

作者信息

Hassard B D, Shiau L J

机构信息

Department of Mathematics SUNY, Buffalo 14214-2093.

出版信息

J Theor Biol. 1989 Feb 8;136(3):267-79. doi: 10.1016/s0022-5193(89)80163-8.

Abstract

Periodic solutions of the current clamped Hodgkin-Huxley equations (Hodgkin & Huxley, 1952 J. Physiol. 117, 500) that arise by degenerate Hopf bifurcation were studied recently by Labouriau (1985 SIAM J. Math. Anal. 16, 1121, 1987 Degenerate Hopf Bifurcation and Nerve Impulse (Part II), in press). Two parameters, temperature T and sodium conductance gNa were varied from the original values obtained by Hodgkin & Huxley. Labouriau's work proved the existence of small amplitude periodic solution branches that do not connect locally to the stationary solution branch, and had not been previously computed. In this paper we compute these solution branches globally. We find families of isolas of periodic solutions (i.e. branches not connected to the stationary branch). For values of gNa in the range measured by Hodgkin & Huxley, and for physically reasonable temperatures, there are isolas containing orbitally asymptotically stable solutions. The presence of isolas of periodic solutions suggests that in certain current space clamped membrane experiments, action potentials could be observed even though the stationary state is stable for all current stimuli. Once produced, such action potentials will disappear suddenly if the current stimulus is either increased or decreased past certain values. Under some conditions, "jumping" between action potentials of different amplitudes might be observed.

摘要

最近,拉博里奥(1985年,《工业与应用数学学会数学分析杂志》第16卷,第1121页;1987年,《退化霍普夫分岔与神经冲动(第二部分)》,即将发表)研究了由退化霍普夫分岔产生的电流钳制霍奇金 - 赫胥黎方程(霍奇金和赫胥黎,1952年,《生理学杂志》第117卷,第500页)的周期解。两个参数,温度T和钠电导gNa,与霍奇金和赫胥黎得到的原始值不同。拉博里奥的工作证明了存在小振幅周期解分支,这些分支在局部不与稳态解分支相连,并且以前没有计算过。在本文中,我们全局计算这些解分支。我们发现了周期解的孤立环族(即不与稳态分支相连的分支)。对于霍奇金和赫胥黎测量范围内的gNa值以及物理上合理的温度,存在包含轨道渐近稳定解的孤立环。周期解孤立环的存在表明,在某些电流空间钳制膜实验中,即使稳态对于所有电流刺激都是稳定的,也可能观察到动作电位。一旦产生,当电流刺激增加或减少超过某些值时,这种动作电位将突然消失。在某些条件下,可能会观察到不同幅度动作电位之间的“跳跃”。

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