» Articles » PMID: 14062458

THE SQUID GIANT AXON. MATHEMATICAL MODELS

Overview
Journal Biophys J
Publisher Cell Press
Specialty Biophysics
Date 1963 Sep 1
PMID 14062458
Citations 24
Authors
Affiliations
Soon will be listed here.
Abstract

The voltage clamp results of Hodgkin and Huxley have been reanalyzed in terms of alternative mathematical models. The model used for the potassium conductance changes is similar to that of the HH model except that an empirical functional relationship replaces the fourth power Law used by HH and the twenty-fifth power law used by Cole and Moore. The model used for the sodium conductance changes involves the explicit use of one variable only rather than the two variables m and h of HH. The rise and fall of the sodium conductance during a depolarizing voltage clamp is obtained by specifying that this one variable satisfies a second order differential equation which results from the coupling of two first order equations. Not only can the adjustable parameters of these models be made to give good fit to the clamp conductance data but the models can also then be used to compute action potential curves. Theoretical interpretations can also be given to these mathematical models.

Citing Articles

A transition state theory approach to the kinetics of conductance changes in excitable membranes.

Tsien R, Noble D J Membr Biol. 2013; 1(1):248-73.

PMID: 24174053 DOI: 10.1007/BF01869785.


A NEW INTERPRETATION OF THE DYNAMIC CHANGES OF THE POTASSIUM CONDUCTANCE IN THE SQUID GIANT AXON.

Tille J Biophys J. 1965; 5:163-71.

PMID: 14268951 PMC: 1367715. DOI: 10.1016/s0006-3495(65)86708-x.


Modeling state-dependent inactivation of membrane currents.

Marom S, Abbott L Biophys J. 1994; 67(2):515-20.

PMID: 7524708 PMC: 1225394. DOI: 10.1016/S0006-3495(94)80518-1.


Molecular mechanism of sodium conductance changes in nerve: the role of electron transfer and energy migration.

Lee C Bull Math Biol. 1983; 45(5):759-80.

PMID: 6317102 DOI: 10.1007/BF02460048.


Gallamine triethiodide-induced modifications of sodium conductance in Myxicola giant axons.

Schauf C, Smith K J Physiol. 1982; 323:157-71.

PMID: 6284914 PMC: 1250350. DOI: 10.1113/jphysiol.1982.sp014066.


References
1.
HODGKIN A, HUXLEY A . Currents carried by sodium and potassium ions through the membrane of the giant axon of Loligo. J Physiol. 1952; 116(4):449-72. PMC: 1392213. DOI: 10.1113/jphysiol.1952.sp004717. View

2.
Tasaki I, Spyropoulos C . Membrane conductance and current-voltage relation in the squid axon under voltage-clamp. Am J Physiol. 1958; 193(2):318-27. DOI: 10.1152/ajplegacy.1958.193.2.318. View

3.
Cole K, Moore J . Ionic current measurements in the squid giant axon membrane. J Gen Physiol. 1960; 44:123-67. PMC: 2195082. DOI: 10.1085/jgp.44.1.123. View

4.
Fitzhugh R . Thresholds and plateaus in the Hodgkin-Huxley nerve equations. J Gen Physiol. 1960; 43:867-96. PMC: 2195039. DOI: 10.1085/jgp.43.5.867. View

5.
HODGKIN A, HUXLEY A . The components of membrane conductance in the giant axon of Loligo. J Physiol. 1952; 116(4):473-96. PMC: 1392209. DOI: 10.1113/jphysiol.1952.sp004718. View