THE SQUID GIANT AXON. MATHEMATICAL MODELS
Overview
Authors
Affiliations
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.
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.
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.