We examine differences between H-3 binding energies obtained by solvin
g the Faddeev equations using standard partial-wave expansion procedur
es and results from solving the Schrodinger equation by means of the c
oupled-rearrangement-channel variational method. Variational bounds ge
nerated from Faddeev solutions for several contemporary, realistic pot
ential models are presented as a function of the number of partial wav
es retained in the potential expansion. We demonstrate that the Faddee
v wave function yields an optimal variational bound for the partial-wa
ve truncated potential from which it is generated, but it does not yie
ld optimal bounds for the full Hamiltonian or when the potential is pa
rtial-wave truncated at a different level. Finally, qualitative differ
ences between H-3 solutions for static models such as the AV14 and RSC
potentials and for momentum-dependent models such as the Nijmegen sof
t-core and Paris potentials are explored, and comparison is made with
solutions for the RSC/TM two-body-force plus three-body-force model.