In thermodynamics, the limit of local stability against phase separation with respect to small fluctuations is clearly defined by the condition that the second derivative of Gibbs free energy is zero. d 2 G d x 2 = 0 {\displaystyle {\operatorname {d} ^{2}\! G \over \operatorname {d} \!
In thermodynamics, the limit of local stability against phase separation with respect to small fluctuations is clearly defined by the condition that the second derivative of Gibbs free energy is zero. d 2 G d x 2 = 0 {\displaystyle {\operatorname {d} ^{2}\! G \over \operatorname {d} \!
Source: Wikipedia "Spinodal" · CC BY-SA 4.0
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