Abstract
Calorimetric measurements on KD2PO4 have been conducted, and the transition is found to be first order with an entropy change at Tc of (0.2407±0.0016)R. The entropy change associated with destruction of the polarization from 0°K to Tc is found to be (0.4234±0.0071)R. It is shown that a mean-field theory of the type proposed by Silsbee, Uehling, and Schmidt can give a good account of the heat capacity and polarization to within about 1°K of Tc, although the latent heat and entropy are not predicted satisfactorily, presumably because of the breakdown of the mean-field approximation close to the transition. Below Tc the divergence in the heat capacity may be argued to be logarithmic in the region closer than 1° to Tc, or to be as 1(TcT)12 in the region Tc2°<T<Tc0.2°. Arguments are offered in favor of the logarithmic divergence.