The contribution of a pi pi-exchange three-body force to the three-nucleon
binding energy is calculated in terms of a pi N amplitude. The latter is ba
sed on a meson-theoretical model of pi N interaction developed by the Julic
h group. Similar to a previous study based on simple phenomenological pi N
potentials a very small effect of the resulting three-body force is found.
Possible origins of the two-orders-of-magnitude discrepancy between the pre
sent result and the values obtained for the Tucson-Melbourne three-body for
ce are investigated. Evidence is provided that this discrepancy is most lik
ely due to strikingly different off-shell properties of the pi N amplitudes
underlying the two approaches.