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Abstract

In their well-known work, Hodgkin and Huxley considered the following model for nerve impulse transmission across an axon:

$$ \frac{{\partial V}}{{\partial t}} - \frac{{{\partial ^2}V}}{{\partial {x^2}}} = {g_{Na}}{m^3}h\left( {{V_{Na}} - V} \right) + {g_K}{n^4}\left( {{V_K} - V} \right) + {g_L}\left( {{V_L} - V} \right) $$
(1)
$$ \frac{{\partial m}}{{\partial t}} = \left( {{m_\infty } - m} \right)/{T_m} $$
(2)
$$ \frac{{\partial h}}{{\partial t}}=\left({{h_\infty}-h}\right)/{T_h} $$
(3)
$$\ \frac{{\partial n}}{{\partial t}} = \left( {{n_\infty } - n} \right)/{T_n} $$
(4)

Supported by NSF Grant No.DMS 9207064

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© 1993 Springer Science+Business Media Dordrecht

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Fitzgibbon, W., Parrott, M., You, Y. (1993). Global Dynamics of Singularly Perturbed Hodgkin-Huxley Equations. In: Goldstein, G.R., Goldstein, J.A. (eds) Semigroups of Linear and Nonlinear Operations and Applications. Springer, Dordrecht. https://doi.org/10.1007/978-94-011-1888-0_8

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  • DOI: https://doi.org/10.1007/978-94-011-1888-0_8

  • Publisher Name: Springer, Dordrecht

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