  The final states for the process $b \rightarrow s\ \gamma$ have been
extensively discussed in the literature. Similarly-detailed analyses for the
case $b \rightarrow s\ gluon$ have not been performed. Generally this process
is searched for in 2-body decays such as ${\rm B}^0 \rightarrow {\rm K}^+
\pi^-$. We present simple arguments to suggest that most of the time the
quark-level process will give rise to final states with rather high
multiplicities. Comments are made about the applicability of these results to
$b \rightarrow d\ gluon$ and hadronic $b\rightarrow u$ decays.
