  Dynamic renormalization group (RG) methods were originally used by Forster,
Nelson and Stephen (FNS) to study the large-scale behaviour of
randomly-stirred, incompressible fluids governed by the Navier-Stokes
equations. Similar calculations using a variety of methods have been performed
since, but have led to a discrepancy in results. In this paper, we carefully
re-examine in $d$-dimensions the approaches used to calculate the renormalized
viscosity increment and, by including an additional constraint which is
neglected in many procedures, conclude that the original result of FNS is
correct. By explicitly using step functions to control the domain of
integration, we calculate a non-zero correction caused by boundary terms which
cannot be ignored. We then go on to analyze how the noise renormalization,
absent in many approaches, contributes an ${\mathcal O}(k^2)$ correction to the
force autocorrelation and show conditions for this to be taken as a
renormalization of the noise coefficient. Following this, we discuss the
applicability of this RG procedure to the calculation of the inertial range
properties of fluid turbulence.
