Titlebook: Mechanics and Energetics of Biological Transport; Erich Heinz Book 1978 Springer-Verlag Berlin · Heidelberg 1978 Energetics.Mechanics.dyna

Emasculate

Nonmediated (Free) Diffusionto the chemical composition and the topographical structure of biological membranes has been gained. Moreover, artificial membranes are now available to serve as suitable models to study special features of biological membranes. Still, the connections between morphological features and transport beh

膽大

Mediated (“Facilitaded”) Diffusionolute owing to frictional forces. In the present chapter we shall discuss how such interactions may, under special conditions, greatly accelerate the penetration. Apparently such interaction involves a specific component of the membrane, which in essence functions as a “mediator” of the translocatio

Blood-Vessels

Isotope Interaction — Tracer Couplingith fixed of mobile membrane constituents (solute-membrane interactions), have been disregarded. In biological membranes, however, a penetrating solute particle is likely to interact with other moving particles, either of the same, or of a different solute species. Such interactions may be direct, e

Sputum

Energetics of One-Flow Systems Treatment of One-Flow Systems in Terms of Thermodynamics of Irreversie the treatment according to the LMA. The flow of a single solute, in the absence of nonconjugate forces, should be proportional to the conjugate driving ., and inversely proportional to a resistance coefficient. The force is conventionally defined as the gradient of the electrochemical potential of

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Phase-Specific Forcessport of a single solute species. These driving forces originated from electrochemical potential gradients or from affinities of reactions that were stoichiometrically coupled to the transport system, usually via a solute-specific carrier mechanism.

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柔聲地說

Mechanics and Energetics of Biological Transport978-3-642-81259-0Series ISSN 0077-0221