An analysis of the thermodynamics of protein stability reveals a general tendency for proteins that denature at higher temperatures to have greater free energies of maximal stability. To a reasonable approximation, the temperature of maximal stability for the set of globular, water-soluble proteins surveyed by Robertson and Murphy occurs at T* ∼283K, independent of the heat denaturation temperature, T m . This observation indicates, at least for these proteins, that thermostability tends to be achieved through elevation of the stability curve rather than by broadening or through a horizontal shift to higher temperatures. The relationship between the free energy of maximal stability and the temperature of heat denaturation is such that an increase in maximal stability of ∼0.008 kJ/mole/residue is, on average, associated with a 1°C increase in T m . An estimate of the energetic consequences of thermal expansion suggests that these effects may contribute significantly to the destabilization of the native state of proteins with increasing temperature.Keywords: Protein stability; thermal expansion; protein volumes; stability curveThe temperature dependence of the free energy change, ⌬G(T), for protein unfolding:under a given set of conditions (pH, ionic strength, reduction potential, etc.) may be conveniently represented by the stability curve (Becktel and Schellman 1987) as depicted in Figure 1. When the heat capacity is temperature independent, the stability curve is determined by the values of three parameters, T m , ⌬H m , and ⌬C p through the relationship (Hawley 1971;Privalov and Gill 1988):in which T m is the temperature of heat denaturation with ⌬G(T m ) ס 0; ⌬H m is the enthalpy of unfolding at T m ; ⌬C p is the heat capacity change on unfolding. The positive ⌬C p of protein denaturation likely reflects the exposure to water of hydrophobic groups that were buried in the native state. One consequence of ⌬C p > 0 is that the stability curve is indeed a curve (Brandts 1964), and it shows a free energy of maximal stability at a temperature T*. In addition to T m , there is a second point on the stability curve where ⌬G is also equal to zero that corresponds to the phenomenon of cold denaturation (Privalov 1990). The stability curve may be approximated as a quadratic function of the temperature with a free energy of maximal stability occurring at a temperature T* (Zipp and Kauzmann 1973;Stowell and Rees 1995), in which: