Local compositional stability requires positive curvature of the mixing free energy. Differentiating twice at fixed temperature, with independent of composition as in the given model, gives
The spinodal occurs where this vanishes:
Between the two spinodal compositions at sufficiently large , and a homogeneous mixture is unstable to infinitesimal composition fluctuations. The binodal is instead fixed by the common-tangent construction, and encloses a larger coexistence region. Between binodal and spinodal the mixture is locally stable but metastable.
A phase diagram with a conventional upper critical temperature additionally assumes that decreases with , for example with . Then high temperature gives a uniform mixture; cooling produces an asymmetric coexistence dome whose critical composition is on the dilute-polymer side. The spinodal lies inside the binodal dome. An arbitrary need not give this orientation, so the free-energy formula alone does not specify a unique temperature axis.
Figure 1. . Original calculations for with the illustrative law . Left: binodal, spinodal and critical point near the critical temperature; horizontal dotted lines mark the two temperatures used in part (e). The other panels show free energies above and below the critical temperature after subtraction of affine references: the tangent at for the upper temperature and the common tangent for the lower temperature. These subtractions leave phase stability and coexistence unchanged. The low-temperature panel displays the common tangent and spinodal boundaries. Details.

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