» Articles » PMID: 5434647

The Sodium-potassium Exchange Pump: Relation of Metabolism to Electrical Properties of the Cell. I. Theory

Overview
Journal Biophys J
Publisher Cell Press
Specialty Biophysics
Date 1970 Mar 1
PMID 5434647
Citations 13
Authors
Affiliations
Soon will be listed here.
Abstract

The Na-K exchange pump is represented as a net stoichiometrically coupled reaction, r, involving ATP, Na(+), and K(+), and is located in the active region of the cell membrane. The reaction rate is J(r) = L(rr) (-DeltaF(r)), where DeltaF(r) is the free energy change of the reaction. DeltaF(r) includes membrane potential ø(2) in the absence of 1:1 coupling between Na(+) and K(+), and the reaction rate is potential dependent under these conditions. At the same time the pump will produce a potential H which is the difference between membrane potential and the diffusion potential as calculated with constant field assumptions. In the absence of 1:1 coupling, the pump is electrogenic. The feedback relation between reaction rate and membrane potential makes the membrane resistance in the presence of the pump less than or equal to the resistance in its absence, at the same membrane potential. H depends on stoichiometry, reaction rate, and passive ionic conductances. Experimental verification of the model will depend on the accuracy of permeability determinations. Dissipation and efficiency of transport can be calculated also.

Citing Articles

A Thermodynamic Model of Monovalent Cation Homeostasis in the Yeast Saccharomyces cerevisiae.

Gerber S, Frohlich M, Lichtenberg-Frate H, Shabala S, Shabala L, Klipp E PLoS Comput Biol. 2016; 12(1):e1004703.

PMID: 26815455 PMC: 4729481. DOI: 10.1371/journal.pcbi.1004703.


Stimulation of a ouabain-sensitive Rb+ uptake in human erthrocytes with an external electric field.

Serpersu E, Tsong T J Membr Biol. 1983; 74(3):191-201.

PMID: 6887232 DOI: 10.1007/BF02332123.


Simulated tetanic hyperpolarization by sodium loading of a neuronal system in which active transport is linked to the Frankenhaeuser-Huxley equations.

SCHOEPFLE G, Tarvin J, Martin R Bull Math Biol. 1983; 45(6):1013-28.

PMID: 6661588 DOI: 10.1007/BF02458828.


Electrical and biochemical properties of an enzyme model of the sodium pump.

Chapman J, Johnson E, Kootsey J J Membr Biol. 1983; 74(2):139-53.

PMID: 6308260 DOI: 10.1007/BF01870503.


Mosaic nonequilibrium thermodynamics describes biological energy transduction.

Westerhoff H, Hellingwerf K, Arents J, Scholte B, van Dam K Proc Natl Acad Sci U S A. 1981; 78(6):3554-8.

PMID: 6267598 PMC: 319608. DOI: 10.1073/pnas.78.6.3554.


References
1.
Garrahan P, Glynn I . The stoicheiometry of the sodium pump. J Physiol. 1967; 192(1):217-35. PMC: 1365482. DOI: 10.1113/jphysiol.1967.sp008297. View

2.
Keynes R . The ionic fluxes in frog muscle. Proc R Soc Lond B Biol Sci. 1954; 142(908):359-82. DOI: 10.1098/rspb.1954.0030. View

3.
Kernan R . Membrane potential changes during sodium transport in frog sartorius muscle. Nature. 1962; 193:986-7. DOI: 10.1038/193986a0. View

4.
Heinz E, PATLAK C . Energy expenditure by active transport mechanisms. Biochim Biophys Acta. 1960; 44:324-34. DOI: 10.1016/0006-3002(60)91568-7. View

5.
CROSS S, Keynes R, RYBOVA R . The coupling of sodium efflux and potassium influx in frog muscle. J Physiol. 1965; 181(4):865-80. PMC: 1357688. DOI: 10.1113/jphysiol.1965.sp007802. View