  Drawing analogy of replacing the nucleon by heavy chiral quark $Q$, the pion
by Goldstone boson $G$, and $\pi NN$ coupling by $GQQ$ coupling, we construct a
statistical model for $Q\bar Q \to nG$ annihilation, i.e. into $n$ longitudinal
weak bosons. This analogy is becoming prescient since the LHC direct bound $m_Q
> 611$ GeV implies strong Yukawa coupling. Taking $m_Q \in (1, 2)$ TeV, the
mean number $<n_G>$ ranges from 6 to over 10, with negligible two or three
boson production. With individual $t'$ or $b'$ decays suppressed either by
phase space or quark mixing, and given the strong Yukawa coupling, $Q\bar Q\to
nV_L$ is the likely outcome for very heavy $Q\bar Q$ production at the LHC.
