  A particular choice of renormalization, within the simplifications provided
by the non-perturbative property of Effective Locality, leads to a completely
finite, renormalized theory of QCD, in which all correlation functions can, in
principle, be defined and calculated. In this Model of renormalization, only
the Bundle chain-Graphs of the cluster expansion are non-zero. All Bundle
graphs connecting to closed quark loops of whatever complexity, and attached to
a single quark line, provided no 'self-energy' to that quark line, and hence no
effective renormalization. However, the exchange of momentum between one quark
line and another, involves only the cluster-expansion's chain graphs, and
yields a set of contributions which can be summed and provide a finite
color-charge renormalization that can be incorporated into all other QCD
processes. An application to high energy elastic pp scattering is now underway.
