  We discuss monopoles formed due to the spontaneous breakdown of a global
$SO(3)_{\rm HF}$ symmetry within the global two-Higgs doublet model. We explain
that the Higgs sector dynamics can be described in terms of two vectors one of
which is null, $R^A=(R^0,R^a,R^4,R^5)$ for $a=1,2,3$, with 5 independent
components describing the Higgs family symmetry and another, $n^a$, with 3
independent components related to the ``would-be'' Goldstone bosons. When
formed from random initial conditions we find that monopoles are formed with a
charged vacuum in the centre which couples the two fields together. We find a
spherical symmetric solution which is an approximately uniform, unit winding of
the sphere in both the $R^a$ and $n^a$ vectors. These global monopoles are
closely related to the Nambu monopole. The additional complexity and structure
contained in these monopoles does not appear to prevent the scaling of their
density.
