A simple phenomenology is developed for the decay and transport of tur
bulence in a constant-speed, uniformly expanding medium. The fluctuati
ons are assumed to be locally incompressible, and either of the hydrod
ynamic or non-Alfvenic magnetohydrodynamic (MHD) type. In order to rep
resent local effects of nonlinearities, a simple model of the Karman-D
ryden type for locally homogeneous turbulent decay is adopted. A detai
led discussion of the parameters of this familiar one-point hydrodynam
ic closure is given, which has been shown recently to be applicable to
non-Alfvenic MHD as well. The effects of the large-scale flow and exp
ansion are incorporated using a two-scale approach, in which assumptio
ns of particular turbulence symmetries provide simplifications. The de
rived model is tractable and provides a basis for understanding turbul
ence in the outer heliosphere: as well as in other astrophysical appli
cations.