Cargando…
Relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle
Activation of skeletal muscle fibers requires rapid sarcolemmal action potential (AP) conduction to ensure uniform excitation along the fiber length, as well as successful tubular excitation to initiate excitation–contraction coupling. In our companion paper in this issue, Pedersen et al. (2011. J....
Autores principales: | , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Rockefeller University Press
2011
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3135325/ https://www.ncbi.nlm.nih.gov/pubmed/21670205 http://dx.doi.org/10.1085/jgp.201110617 |
_version_ | 1782208084896120832 |
---|---|
author | Fraser, James A. Huang, Christopher L.-H. Pedersen, Thomas H. |
author_facet | Fraser, James A. Huang, Christopher L.-H. Pedersen, Thomas H. |
author_sort | Fraser, James A. |
collection | PubMed |
description | Activation of skeletal muscle fibers requires rapid sarcolemmal action potential (AP) conduction to ensure uniform excitation along the fiber length, as well as successful tubular excitation to initiate excitation–contraction coupling. In our companion paper in this issue, Pedersen et al. (2011. J. Gen. Physiol. doi:10.1085/jgp.201010510) quantify, for subthreshold stimuli, the influence upon both surface conduction velocity and tubular (t)-system excitation of the large changes in resting membrane conductance (G(M)) that occur during repetitive AP firing. The present work extends the analysis by developing a multi-compartment modification of the charge–difference model of Fraser and Huang to provide a quantitative description of the conduction velocity of actively propagated APs; the influence of voltage-gated ion channels within the t-system; the influence of t-system APs on ionic homeostasis within the t-system; the influence of t-system ion concentration changes on membrane potentials; and the influence of Phase I and Phase II G(M) changes on these relationships. Passive conduction properties of the novel model agreed with established linear circuit analysis and previous experimental results, while key simulations of AP firing were tested against focused experimental microelectrode measurements of membrane potential. This study thereby first quantified the effects of the t-system luminal resistance and voltage-gated Na(+) channel density on surface AP propagation and the resultant electrical response of the t-system. Second, it demonstrated the influence of G(M) changes during repetitive AP firing upon surface and t-system excitability. Third, it showed that significant K(+) accumulation occurs within the t-system during repetitive AP firing and produces a baseline depolarization of the surface membrane potential. Finally, it indicated that G(M) changes during repetitive AP firing significantly influence both t-system K(+) accumulation and its influence on the resting membrane potential. Thus, the present study emerges with a quantitative description of the changes in membrane potential, excitability, and t-system ionic homeostasis that occur during repetitive AP firing in skeletal muscle. |
format | Online Article Text |
id | pubmed-3135325 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2011 |
publisher | The Rockefeller University Press |
record_format | MEDLINE/PubMed |
spelling | pubmed-31353252012-01-01 Relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle Fraser, James A. Huang, Christopher L.-H. Pedersen, Thomas H. J Gen Physiol Article Activation of skeletal muscle fibers requires rapid sarcolemmal action potential (AP) conduction to ensure uniform excitation along the fiber length, as well as successful tubular excitation to initiate excitation–contraction coupling. In our companion paper in this issue, Pedersen et al. (2011. J. Gen. Physiol. doi:10.1085/jgp.201010510) quantify, for subthreshold stimuli, the influence upon both surface conduction velocity and tubular (t)-system excitation of the large changes in resting membrane conductance (G(M)) that occur during repetitive AP firing. The present work extends the analysis by developing a multi-compartment modification of the charge–difference model of Fraser and Huang to provide a quantitative description of the conduction velocity of actively propagated APs; the influence of voltage-gated ion channels within the t-system; the influence of t-system APs on ionic homeostasis within the t-system; the influence of t-system ion concentration changes on membrane potentials; and the influence of Phase I and Phase II G(M) changes on these relationships. Passive conduction properties of the novel model agreed with established linear circuit analysis and previous experimental results, while key simulations of AP firing were tested against focused experimental microelectrode measurements of membrane potential. This study thereby first quantified the effects of the t-system luminal resistance and voltage-gated Na(+) channel density on surface AP propagation and the resultant electrical response of the t-system. Second, it demonstrated the influence of G(M) changes during repetitive AP firing upon surface and t-system excitability. Third, it showed that significant K(+) accumulation occurs within the t-system during repetitive AP firing and produces a baseline depolarization of the surface membrane potential. Finally, it indicated that G(M) changes during repetitive AP firing significantly influence both t-system K(+) accumulation and its influence on the resting membrane potential. Thus, the present study emerges with a quantitative description of the changes in membrane potential, excitability, and t-system ionic homeostasis that occur during repetitive AP firing in skeletal muscle. The Rockefeller University Press 2011-07 /pmc/articles/PMC3135325/ /pubmed/21670205 http://dx.doi.org/10.1085/jgp.201110617 Text en © 2011 Fraser et al. 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 3.0 Unported license, as described at http://creativecommons.org/licenses/by-nc-sa/3.0/). |
spellingShingle | Article Fraser, James A. Huang, Christopher L.-H. Pedersen, Thomas H. Relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle |
title | Relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle |
title_full | Relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle |
title_fullStr | Relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle |
title_full_unstemmed | Relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle |
title_short | Relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle |
title_sort | relationships between resting conductances, excitability, and t-system ionic homeostasis in skeletal muscle |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3135325/ https://www.ncbi.nlm.nih.gov/pubmed/21670205 http://dx.doi.org/10.1085/jgp.201110617 |
work_keys_str_mv | AT fraserjamesa relationshipsbetweenrestingconductancesexcitabilityandtsystemionichomeostasisinskeletalmuscle AT huangchristopherlh relationshipsbetweenrestingconductancesexcitabilityandtsystemionichomeostasisinskeletalmuscle AT pedersenthomash relationshipsbetweenrestingconductancesexcitabilityandtsystemionichomeostasisinskeletalmuscle |