  The production of $W^+ W^-$ pair in hadron colliders was calculated up to
loop corrections by some authors in the Electroweak standard model (SM)
framework. This production was also calculated, at the tree level, in some
extensions of the SM such as the vector singlet, the fermion mirror fermion and
the vector doublet models by considering the contributions of new neutral gauge
bosons and exotic fermions. The obtained results for $e^+ e^-$ and $pp$
collisions pointed out that the new physics contributions are quite important.
This motivates us to calculate the production of a more massive charged gauge
boson predicted by the ${SU (3)_C \times SU (3)_L \times U (1)_X}$ model (3-3-1
model). Thus, the aim of the present paper is to analyze the role played by of
the extra gauge boson ${Z^\prime}$ and of the exotic quarks, predicted in the
minimal version of the 3-3-1 model, by considering the inclusive production of
a pair of bileptons ($V^\pm$) in the reaction $p + p \longrightarrow V^+ + V^-
+ X$, at the Large Hadron Collider (LHC) energies.
  Our results show that the correct energy behavior of the elementary cross
section follows from the balance between the contributions of the extra neutral
gauge boson with those from the exotic quarks. The extra neutral gauge boson
induces flavor-changing neutral currents (FCNC) at tree level, and we have
introduced the ordinary quark mixing matrices for the model when the first
family transforms differently to the other two with respect to $SU(3)_L$. We
obtain a huge number of heavy bilepton pairs produced for two different values
of the center of mass energy of the LHC.
