Finite dimensionality and upper semicontinuity of the global attractor of singularly perturbed Hodgkin-Huxley systems (Q1923669)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Finite dimensionality and upper semicontinuity of the global attractor of singularly perturbed Hodgkin-Huxley systems |
scientific article; zbMATH DE number 933274
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Finite dimensionality and upper semicontinuity of the global attractor of singularly perturbed Hodgkin-Huxley systems |
scientific article; zbMATH DE number 933274 |
Statements
Finite dimensionality and upper semicontinuity of the global attractor of singularly perturbed Hodgkin-Huxley systems (English)
0 references
10 October 1996
0 references
The authors consider the Hodgkin-Huxley system \[ {{\partial\nu}\over{\partial t}}-{{\partial^2\nu} \over {\partial x^2}}= g_{N_a}m^3h (\nu_{N_a}-\nu)+ g_Kn^4 (\nu_K-\nu)+ g_L(\nu_L-\nu) \] with some given conditions. Due to the fact that the inductance in this system is small and can be ignored the authors perturb this system to the system \[ \varepsilon {{\partial^2\nu}\over{\partial t^2}}+ (\varepsilon f(m,h)+1) {{\partial\nu}\over{\partial t}}-{{\partial^2\nu}\over {\partial x^2}}= g_{N_a}m^3h (\nu_K-\nu)+ g_Kn^4 (\nu_K-\nu)+ g_L(\nu_L-\nu). \] The solution of the perturbed system is used to approximate the solution of the original system. This article is of many articles on this subject published by the authors. Using normal singular perturbation techniques it is shown that the solution of the perturbed system converges to the solution of the unperturbed system.
0 references
Hodgkin-Huxley system
0 references
perturbed system
0 references
singular perturbation techniques
0 references