The multifragmentation of excited spherical nuclear sources with various N/
Z ratios and fixed mass number is studied within dynamical and statistical
models. The dynamical model treats the multifragmentation process as a fina
l stage of growth of density fluctuations in unstable expanding nuclear mat
ter. The statistical model makes a choice of the final multifragment config
uration according to its statistical weight at a global thermal equilibrium
. Similarities and differences in the predictions of the two models on the
isotopic composition of the produced fragments are presented and the most s
ensitive observable characteristics are discussed. (C) 1999 Elsevier Scienc
e B.V. All rights reserved.