For the measurement of crystallization pressures, Khaimov-Markov (1958) devised a method of disarming simplicity, as shown by the insert in Fig.
3.2.1. Seed crystals of aluminium potassium alum were placed on the top of a gel, with one of the crystal faces in contact with the gel surface. The
gel itself was supersaturated with solute, and as the crystal grew it was lifted up, eventually to a height of several millimetres. By placing weights
on the crystal, the lift could be suppressed, as shown by the graph in Fig. 3.2.\{a). In this way, and by monitoring crystal size, the pressure (i.e.
the thrust per unit area) could be simply determined. This pressure, in turn, was found to be a simple function of the super- saturation (Fig.
3.2.l(b)).
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