  We describe the internal composition of a topologically stable monopole
carrying a magnetic charge of $6\pi/e$ that arises from the spontaneous
breaking of the trinification symmetry $SU(3)_c\times SU(3)_L\times SU(3)_R$
($G$). Since this monopole carries no color magnetic charge, a charge of
$6\pi/e$ is required by the Dirac quantization condition. The breaking of $G$
to the Standard Model occurs in a number of steps and yields the desired
topologically stable monopole ("magnetic baryon"), consisting of three confined
monopoles. The confined monopoles ("magnetic quarks") each carry a combination
of Coulomb magnetic flux and magnetic flux tubes, and therefore they do not
exist as isolated states. We also display a more elaborate configuration ("fang
necklace") composed of these magnetic quarks. In contrast to the $SU(5)$
monopole which is superheavy and carries a magnetic charge of $2\pi/e$ as well
as color magnetic charge, the trinification monopole may have mass in the TeV
range, in which case it may be accessible at the LHC and its planned upgrades.

High Energy Physics - Phenomenology;High Energy Physics - Theory