174 FLUIDITY AND PLASTICITY Case III.—In the usual case in practice, the fluidity-tempera- ture curves are not parallel, so that the fluidities may be identical at one temperature but very different at another. We then obtain a series of curves as shown in Fig. 65a and 65&. At low temperatures there is a good minimum in the fluidity-volume concentration curves, but it gradually shifts to the right as the temperature is raised, until at the highest temperatures it dis- appears altogether. It is manifestly erroneous to assume that the composition of the hydrate changes on this account. On the other hand, the deviation from the expected linear curves as ^^ <*~»?\ a FIG. 65.—Diagram illustrating how the minimum in the fluidity-concentra- tion curve may shift with the temperature. The maximum deviation from the linear curve is the significant quantity. This quantity floes not vary with the temperature and it indicates the composition of the solvate. measured vertically is everywhere the same as in the simpler cases. In practice, the hydration is generally less at the higher temperatures so that the deviation should grow less as the tem- perature is raised, but the cases already given are sufficient to show that the deviation of the observed fluidity-volume concentra- tion curve from the linear curve, which would be expected were there no combination between the components of the solution, can alone furnish trustworthy information. Were the components of the mixture non-associated, it seems possible to calculate not only the composition of the solvate formed but also the percentage of it existing in the solution. But substances which form feeble combinations on mixing are usually themselves associated, and it is quite likely that this