Abstract
Only a rudimentary understanding of the principles of classical thermodynamics is needed to appreciate that the flow of an uncharged substance from a region of lower concentration to a region of higher concentration or the flow of a charged substance from a region of lower electrochemical potential to a region of higher electrochemical potential cannot take place unless the processes responsible for these flows are linked or coupled to a supply of energy. Such flows, loosely referred to as “active” or “uphill,” are commonplace in biological systems and the thrust of many investigations is to identify the immediately responsible source(s) of energy. The problem can perhaps be best stated in terms of the formalism of irreversible or nonequilibrium thermodynamics.(1) Thus, in a system in which there is only a single flow of a substance i we may write the straight phenomenologic coefficient relating the flow to the conjugate force and has units of conductance; R ii relates the force to the flow and has units of resistance. Clearly, in this simple system R ii = 1/L ii . Ohm’s law of current flow, Fick’s first law of diffusion, Fourier’s law of heat flow, and Poiseuille’s law of volume flow are but a few familiar examples of Eq. (1).
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Schultz, S.G. (1978). Ion-Coupled Transport across Biological Membranes. In: Andreoli, T.E., Hoffman, J.F., Fanestil, D.D. (eds) Physiology of Membrane Disorders. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-3958-8_15
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