The energetics of barstar denaturation have been studied by CD and scanning microcalorimetry in an extended range of pH and salt concentration. It was shown that, upon increasing temperature, barstar undergoes a transition to the denatured state that is well approximated by a two-state transition in solutions of high ionic strength. This transition is accompanied by significant heat absorption and an increase in heat capacity. The denaturational heat capacity increment at =75 "C was found to be 5.6 f 0.3 kJ K" mol". In all cases, the value of the measured enthalpy of denaturation was notably lower than those observed for other small globular proteins. In order to explain this observation, the relative contributions of hydration and the disruption of internal interactions to the total enthalpy and entropy of unfolding were calculated. The enthalpy and entropy of hydration were found to be in good agreement with those calculated for other proteins, but the enthalpy and entropy of breaking internal interactions were found to be among the lowest for all globular proteins that have been studied. Additionally, the partial specific heat capacity of barstar in the native state was found to be 0.37 f 0.03 cal K-' gg', which is higher than what is observed for most globular proteins and suggests significant flexibility in the native state. It is known from structural data that barstar undergoes a conformational change upon binding to its natural substrate barnase. Our data, which indicate that barstar has a loosely packed interior, suggest that high conformational flexibility of barstar's native structure may play an important role in allowing it to optimize its contacts with barnase upon binding without disrupting favorable, tightly packed internal interactions.
Keywords: barstar; protein stability; scanning microcalorimetryThe interaction between barnase, the extracellular ribonuclease of Bacillus amyloliquefaciens, and barstar, its natural inhibitor, has attracted a great deal of attention as a good model for the study of protein-protein recognition (Hartley, 1993;Schreiber & Fersht, 1993a). The crystal structure of Cys 40, 82 Ala barstar complexed with barnase was recently solved with a resolution that is sufficient for detailed analysis of the interactions stabilizing the complex (Guillet et al., 1993;Buckle et al., 1994), and the structures of both free barnase (Mauguen et al., 1982;Bycroft et al., 1991) and free barstar (Lubienski et al., 1994) are known. To understand the mechanisms by which these proteins associate with one another, we require knowledge of the thermodynamics of complex formation and the energetics of native structure formation in both free barnase and free barstar. Although the energetics of barnase have been studied in detail by several groups (Hartley, 1%8, 1975; Makarov et al., 1993;Griko et al., 1994;Sanz et al., 1994), the energetics of native barstar are less well understood. The free energy of barstar unfolding by urea was estimated by Schreiber and Fersht (1993b), and the van't Ho...