(1) Assuming that water and ice are incompressible, we can find the decrease in the temperature of the mixture as a result of the increase in the external pressure:
Such a small change in temperature indicates that only a small mass of ice will melt, i.e. Δm << mice.
We write the energy conservation law:
Let us estimate the work A done by the external force. The change in the volume of the mixture as a result of melting ice of mass Δm is
We have taken into account the fact that the density of water decreases as a result of freezing by about 10%, i.e.,
Therefore, we obtain an estimate
The amount of heat ΔQ required fot heating the mass m of ice and the same mass of water by ΔT is
Since A << ΔQ,. we can assume that λ Δm = ΔQ, whence
The change in volume as a result of melting ice of this mass is
Considering that for a slow increase in pressure the change in the volume ΔV, is proportional to that in the pressure Δp, we can find the work clone by the external force:
(2) We now take into account the compressibility of water and ice. The change in the volume of water and ice will be
where V0w, =10-3 m3 and V0ice = 1.1 x 10-3 m3 are the initial volumes of water and ice. The work A done by the external force to compress the mixture is
The total work of the external force is
Obviously, since we again have Atot << ΔQ, the mass of the ice that has melted will be the same as in case (1).