Berland C R, Thurston G M, Kondo M, Broide M L, Pande J, Ogun O, Benedek G B
Department of Physics, Massachusetts Institute of Technology, Cambridge 02139.
Proc Natl Acad Sci U S A. 1992 Feb 15;89(4):1214-8. doi: 10.1073/pnas.89.4.1214.
We report measurement of the solid-liquid phase boundary, or liquidus line, for aqueous solutions of three pure calf gamma-crystallin proteins: gamma II, gamma IIIa, and gamma IIIb. We also studied the liquidus line for solutions of native gamma IV-crystallin calf lens protein, which consists of 85% gamma IVa/15% gamma IVb. In all four proteins the liquidus phase boundaries lie higher in temperature than the previously determined liquid-liquid coexistence curves. Thus, over the range of concentration and temperature for which liquid-liquid phase separation occurs, the coexistence of a protein crystal phase with a protein liquid solution phase is thermodynamically stable relative to the metastable separated liquid phases. The location of the liquidus lines clearly divides these four crystallin proteins into two groups: those in which liquidus lines flatten at temperatures greater than 70 degrees C: gamma IIIa and gamma IV, and those in which liquidus lines flatten at temperatures less than 50 degrees C: gamma II and gamma IIIb. We have analyzed the form of the liquidus lines by using specific choices for the structures of the Gibbs free energy in solution and solid phases. By applying the thermodynamic conditions for equilibrium between the two phases to the resulting chemical potentials, we can estimate the temperature-dependent free energy change upon binding of protein and water into the solid phase.
我们报告了三种纯小牛γ-晶状体蛋白(γII、γIIIa和γIIIb)水溶液的固-液相边界(即液相线)的测量结果。我们还研究了天然γIV-晶状体小牛晶状体蛋白溶液的液相线,该蛋白由85%的γIVa/15%的γIVb组成。在所有这四种蛋白质中,液相线的温度高于先前确定的液-液共存曲线。因此,在发生液-液相分离的浓度和温度范围内,相对于亚稳态的分离液相,蛋白质晶相与蛋白质液相溶液相的共存是热力学稳定的。液相线的位置清楚地将这四种晶状体蛋白分为两组:液相线在温度高于70℃时变平的蛋白:γIIIa和γIV;以及液相线在温度低于50℃时变平的蛋白:γII和γIIIb。我们通过对溶液相和固相中吉布斯自由能的结构进行特定选择来分析液相线的形式。通过将两相之间平衡的热力学条件应用于所得的化学势,我们可以估计蛋白质和水结合进入固相时随温度变化的自由能变化。