Structure and Energetics of the Hydrogen-Bonded Backbone in Protein Folding

Author:

Bolen D. Wayne1,Rose George D.2

Affiliation:

1. Department of Biochemistry and Molecular Biology and The Sealy Center for Structural Biology, The University of Texas Medical Branch, Galveston, Texas 77555-1052;

2. T.C. Jenkins Department of Biophysics, Johns Hopkins University, Baltimore, Maryland 21218;

Abstract

We seek to understand the link between protein thermodynamics and protein structure in molecular detail. A classical approach to this problem involves assessing changes in protein stability resulting from added cosolvents. Under any given conditions, protein molecules in aqueous buffer are in equilibrium between unfolded and folded states, U(nfolded) [Formula: see text] N(ative). Addition of organic osmolytes, small uncharged compounds found throughout nature, shift this equilibrium. Urea, a denaturing osmolyte, shifts the equilibrium toward U; trimethylamine N-oxide (TMAO), a protecting osmolyte, shifts the equilibrium toward N. Using the Tanford Transfer Model, the thermodynamic response to many such osmolytes has been dissected into groupwise free energy contributions. It is found that the energetics involving backbone hydrogen bonding controls these shifts in protein stability almost entirely, with osmolyte cosolvents simply dialing between solvent-backbone versus backbone-backbone hydrogen bonds, as a function of solvent quality. This reciprocal relationship establishes the essential link between protein thermodynamics and the protein's hydrogen-bonded backbone structure.

Publisher

Annual Reviews

Subject

Biochemistry

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