The unified site relaxation model combines key features of the earlier
dynamic structure and jump relaxation models, and provides a coherent
model of ionic transport processes in glassy materials. The essential
idea is that mobile ions hop backwards and forwards many times before
: (i) the Coulomb field is relaxed and (ii) the 'target site' adjusts
itself to the needs of its new occupant. The other mobile ions and the
network of the glass are both involved in this (unified) relaxation p
rocess. Manifestations of site relaxation are seen in the frequency de
pendence of the conductivity, in mechanical loss spectra and in many d
.c. 'anomalies' such as the mixed cation effect.