Abstract

The MWC (Monod–Wyman–Changeux) allosteric model postulates concerted conformational changes between two states: the intrinsically more stable T state with relatively weak ligand binding and the R state with relatively strong ligand binding. The model distinguishes between Y¯ (the fractional occupation of the binding sites) and R¯ (the fraction of molecules in the R state). Cooperativity (measured by the Hill coefficient) has strikingly different properties for Y¯ and R¯. For the latter, cooperativity depends only on the relative affinities of the two states, not on their relative intrinsic stabilities, as demonstrated here with a simple new equation relating the Hill coefficient to R¯.

Highlights

  • The concept of allosteric interactions, introduced a half-century ago [1,2,3], has had a powerful impact in biology for problems of signal transduction and control at various levels [4,5,6,7]

  • The generalization of allostery is reflected by the fact that, some 50 years after creation of this neologism, “allosteric” as a keyword generates over 18,000 responses in PubMed

  • The original mathematical formulation in the MWC (Monod–Wyman–Changeux) model for allosteric proteins is based on two distinct conformational states (T and R) related by a single intrinsic equilibrium constant, L, where L = [T]/[R] in the absence of ligands for that protein [3]

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Summary

Introduction

The concept of allosteric interactions, introduced a half-century ago [1,2,3], has had a powerful impact in biology for problems of signal transduction and control at various levels [4,5,6,7]. Cooperativity depends only on the relative affinities of the two states, not on their relative intrinsic stabilities, as demonstrated here with a simple new equation relating the Hill coefficient toR. Cooperativity of the Allosteric State Function equation for the Hill coefficient of R , which is presented here.

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