Protein hydration, thermodynamic binding, and preferential hydration
Protein hydration, thermodynamic binding, and preferential hydration
复制标题
DOI:
10.1021/bi020316e
复制
发表时间:
2002-11-19
期刊:
影响因子:
2.9
通讯作者:
Timasheff, SN
中科院分区:
文献类型:
--
作者:
Timasheff, SN
The question of protein hydration, ie, the interaction of protein molecules with water, and of the involvement of water molecules in protein reactions has been a focus of attention for the good part of a century. Yet the number of water molecules that interact with one protein molecule, WH (waters of hydration), has been an elusive quantity, notwithstanding measurements by transport (1, 2) and NMR (3) techniques. The reason for this lies in the essence of the physical phenomenon of protein hydration. The fact is that there is no rigid shell of water around a protein molecule, but rather there is a fluctuating cloud of water molecules that are thermodynamically affected more or less strongly by the protein molecule. Nevertheless, the description of the overall effect in terms of an effective number of whole water molecules, WH, has been a useful concept, analogous to the electrostatic double layer representation of the ionic distribution in the cloud around a central ion in the Debye-Hückel theory (4), or the surface of shear used in the analysis of transport phenomena (sedimentation, electrophoresis, diffusion)(5).It is characteristic of protein reactions that, during the course of the reaction, the total surface area of the protein in contact with water changes. This must be accompanied by a change in the number of water molecules with which it interacts, ie, its extent of hydration, ΔWH) WH (product)-WH (reactant). This is true of allosteric transitions, protein