The structural origin of the decrease in system volume upon protein denaturation by pressure has remained a puzzle for decades. This negative volume change upon unfolding is assumed to arise globally from more intimate interactions between the polypeptide chain and water, including electrostriction of buried charges that become exposed upon unfolding, hydration of the polypeptide backbone and amino acid side chains and elimination of packing defects and internal void volumes upon unfolding of the chain. However, the relative signs and magnitudes of each of these contributing factors have not been experimentally determined. Our laboratory has probed the fundamental basis for the volume change upon unfolding of staphylococcal nuclease (Snase) using variable solution conditions and point mutants of Snase (Royer CA et al., 1993, Biochemistry 325222-5232; Frye KJ et al., 1996, Biochemistry 35:10234-10239). Our prior results indicate that for Snase, neither electrostriction nor polar or nonpolar hydration contributes significantly to the value of the volume change of unfolding. In the present work, we investigate the pressure induced unfolding of three point mutants of Snase in which internal cavity size is altered. The experimentally determined volume changes of unfolding for the mutants suggest that loss of internal void volume upon unfolding represents the major contributing factor to the value of the volume change of Snase unfolding.Keywords: high pressure; protein folding; staphylococcal nuclease; volume change Understanding protein folding remains one of the most challenging problems in modem molecular biophysics. Considerable progress has been made in the last decade in the characterization of the fundamental thermodynamic and kinetic aspects of the process, as well as in the structural characterization of the various states, native, intermediate, and unfolded, implicated in the transitions. From a thermodynamic point of view, the fundamental parameter in protein temperature stability, the heat capacity change at constant pressure, which is responsible for the temperature dependence of the entropy, enthalpy, and free energy of folding, has been parameterized and can now be modeled adequately, in terms of the changes in exposure of hydrophobic and hydrophilic moieties of particular proteins based on their sequences and structures (Privalov & Gill, 1988;Murphy & Freire, 1992).Athorough understanding of the thermodynamics of protein folding requires, in addition to the temperature effects, a fundamental comprehension of pressure effects as well. However, in terms of the behavior of proteins under pressure, our level of understanding is much less advanced than in the field of temperature denaturation. (For reviews of pressure effects on proteins see Jaenicke, 1981; HerReprint requests to: Catherine A. Royer, Centre de Biochimie Structurale, INSERM U414, Facultt de Pharmacie, 15 ave. Ch. Flahault, 34060 Montpellier CEDEX, France; e-mail: royer@tome.cbs.univ-montpl.fr. emans, 1982;Weber & Drickamer, 1983;Si...