MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON
The direct current longitudinal resistance of the squid giant axon was measured as a function of the electrode separation. Large sea water electrodes were used and the inter-electrode length was immersed in oil. The slope of the resistance vs. separation curve is large for a small electrode separat...
Main Authors: | , |
---|---|
Format: | Online |
Language: | English |
Published: |
The Rockefeller University Press
1939
|
Online Access: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2142005/ |
id |
pubmed-2142005 |
---|---|
recordtype |
oai_dc |
spelling |
pubmed-21420052008-04-23 MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON Cole, Kenneth S. Hodgkin, Alan L. Article The direct current longitudinal resistance of the squid giant axon was measured as a function of the electrode separation. Large sea water electrodes were used and the inter-electrode length was immersed in oil. The slope of the resistance vs. separation curve is large for a small electrode separation, but becomes smaller and finally constant as the separation is increased. An analysis of the resistance vs. length curves gives the following results. The nerve membrane has a resistance of about 1000 ohm cm.2 The protoplasm has a specific resistance of about 1.4 times that of sea water. The resistance of the connective tissue sheath outside the fiber corresponds to a layer of sea water about 20µ in thickness. The characteristic length for the axon is about 2.3 mm. in oil and 6.0 mm. in sea water. The Rockefeller University Press 1939-05-20 /pmc/articles/PMC2142005/ /pubmed/19873126 Text en Copyright © Copyright, 1939, by The Rockefeller Institute for Medical Research 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/). |
repository_type |
Open Access Journal |
institution_category |
Foreign Institution |
institution |
US National Center for Biotechnology Information |
building |
NCBI PubMed |
collection |
Online Access |
language |
English |
format |
Online |
author |
Cole, Kenneth S. Hodgkin, Alan L. |
spellingShingle |
Cole, Kenneth S. Hodgkin, Alan L. MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON |
author_facet |
Cole, Kenneth S. Hodgkin, Alan L. |
author_sort |
Cole, Kenneth S. |
title |
MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON |
title_short |
MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON |
title_full |
MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON |
title_fullStr |
MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON |
title_full_unstemmed |
MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON |
title_sort |
membrane and protoplasm resistance in the squid giant axon |
description |
The direct current longitudinal resistance of the squid giant axon was measured as a function of the electrode separation. Large sea water electrodes were used and the inter-electrode length was immersed in oil. The slope of the resistance vs. separation curve is large for a small electrode separation, but becomes smaller and finally constant as the separation is increased. An analysis of the resistance vs. length curves gives the following results. The nerve membrane has a resistance of about 1000 ohm cm.2 The protoplasm has a specific resistance of about 1.4 times that of sea water. The resistance of the connective tissue sheath outside the fiber corresponds to a layer of sea water about 20µ in thickness. The characteristic length for the axon is about 2.3 mm. in oil and 6.0 mm. in sea water. |
publisher |
The Rockefeller University Press |
publishDate |
1939 |
url |
https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2142005/ |
_version_ |
1611422961354407936 |