Abstract
The relation ΔCp Δκ = TV(Δα)2 is shown to be obeyed under the same assumptions that Davies and Jones used to derive the weaker condition ΔCp Δκ ≥ TV(Δα)2. This means that if a material is found experimentally not to obey the above equality, then it is not describable by an order‐parameter theory. A prescription is given which allows one to determine within the context of order‐parameter theory whether the glass transition of a given material is basically thermodynamic or kinetic in origin.

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