  We consider the implications of an extended color group, $SU\left( 3\right)
_I\times SU\left( 3\right) _{II}$, spontaneously broken to $SU\left( 3\right)
_c$ at a TeV or lower scale, for the hadronic colliders. The associated massive
color octet gauge bosons (the colorons) can enhance the $t \overline{t}$ pair
production at the Tevatron collider. At the LHC, the colorons can be pair
produced, each decaying to a $t\overline{t}$ pair. This gives rise to anomalous
multi W production: a clear signature of physics beyond the Standard Model. We
calculate the associated multijet and multilepton final states at the Tevatron
and the LHC energies, and compare these with the expectations from the Standard
Model.
