The formalism to include a three-nucleon force into three-nucleon cont
inuum calculations is presented. First numerical results, obtained in
momentum space, are shown. The two- and three-nucleon forces have been
restricted to act only in the S-1(0) and S-3(1)-3D1 partial-wave stat
es. As two-nucleon interaction the Bonn-B potential and as three-nucle
on interaction the Tucson-Melbourne two-pion exchange model has been u
sed.