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Subthreshold Behavior and Phenomenological Impedance of the Squid Giant Axon
The oscillatory behavior of the cephalopod giant axons in response to an applied current has been established by previous investigators. In the study reported here the relationship between the familiar "RC" electrotonic response and the oscillatory behavior is examined experimentally and s...
Autores principales: | , , , |
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Formato: | Texto |
Lenguaje: | English |
Publicado: |
The Rockefeller University Press
1970
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2203007/ https://www.ncbi.nlm.nih.gov/pubmed/5435782 |
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author | Mauro, A. Conti, F. Dodge, F. Schor, R. |
author_facet | Mauro, A. Conti, F. Dodge, F. Schor, R. |
author_sort | Mauro, A. |
collection | PubMed |
description | The oscillatory behavior of the cephalopod giant axons in response to an applied current has been established by previous investigators. In the study reported here the relationship between the familiar "RC" electrotonic response and the oscillatory behavior is examined experimentally and shown to be dependent on the membrane potential. Computations based on the three-current system which was inferred from electrical measurements by Hodgkin and Huxley yield subthreshold responses in good agreement with experimental data. The point which is developed explicitly is that since the three currents, in general, have nonzero resting values and two currents, the "Na" system and the "K" system, are controlled by voltage-dependent time-variant conductances, the subthreshold behavior of the squid axon in the small-signal range can be looked upon as arising from phenomenological inductance or capacitance. The total phenomenological impedance as a function of membrane potential is derived by linearizing the empirically fitted equations which describe the time-variant conductances. At the resting potential the impedance consists of three structures in parallel, namely, two series RL elements and one series RC element. The true membrane capacitance acts in parallel with the phenomenological elements, to give a total impedance which is, in effect, a parallel R, L, C system with a "natural frequency" of oscillation. At relatively hyperpolarized levels the impedance "degenerates" to an RC system. |
format | Text |
id | pubmed-2203007 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 1970 |
publisher | The Rockefeller University Press |
record_format | MEDLINE/PubMed |
spelling | pubmed-22030072008-04-23 Subthreshold Behavior and Phenomenological Impedance of the Squid Giant Axon Mauro, A. Conti, F. Dodge, F. Schor, R. J Gen Physiol Article The oscillatory behavior of the cephalopod giant axons in response to an applied current has been established by previous investigators. In the study reported here the relationship between the familiar "RC" electrotonic response and the oscillatory behavior is examined experimentally and shown to be dependent on the membrane potential. Computations based on the three-current system which was inferred from electrical measurements by Hodgkin and Huxley yield subthreshold responses in good agreement with experimental data. The point which is developed explicitly is that since the three currents, in general, have nonzero resting values and two currents, the "Na" system and the "K" system, are controlled by voltage-dependent time-variant conductances, the subthreshold behavior of the squid axon in the small-signal range can be looked upon as arising from phenomenological inductance or capacitance. The total phenomenological impedance as a function of membrane potential is derived by linearizing the empirically fitted equations which describe the time-variant conductances. At the resting potential the impedance consists of three structures in parallel, namely, two series RL elements and one series RC element. The true membrane capacitance acts in parallel with the phenomenological elements, to give a total impedance which is, in effect, a parallel R, L, C system with a "natural frequency" of oscillation. At relatively hyperpolarized levels the impedance "degenerates" to an RC system. The Rockefeller University Press 1970-04-01 /pmc/articles/PMC2203007/ /pubmed/5435782 Text en Copyright © 1970 by The Rockefeller University Press This article is distributed under the terms of an Attribution–Noncommercial–Share Alike–No Mirror Sites license for the first six months after the publication date (see http://www.rupress.org/terms). After six months it is available under a Creative Commons License (Attribution–Noncommercial–Share Alike 4.0 Unported license, as described at http://creativecommons.org/licenses/by-nc-sa/4.0/). |
spellingShingle | Article Mauro, A. Conti, F. Dodge, F. Schor, R. Subthreshold Behavior and Phenomenological Impedance of the Squid Giant Axon |
title | Subthreshold Behavior and Phenomenological Impedance of the Squid Giant Axon |
title_full | Subthreshold Behavior and Phenomenological Impedance of the Squid Giant Axon |
title_fullStr | Subthreshold Behavior and Phenomenological Impedance of the Squid Giant Axon |
title_full_unstemmed | Subthreshold Behavior and Phenomenological Impedance of the Squid Giant Axon |
title_short | Subthreshold Behavior and Phenomenological Impedance of the Squid Giant Axon |
title_sort | subthreshold behavior and phenomenological impedance of the squid giant axon |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2203007/ https://www.ncbi.nlm.nih.gov/pubmed/5435782 |
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