We study the effective diffusivity tensor for particles in a random gr
adient flow that, statistically, lacks rotational symmetry. The effect
ive diffusivity tensor is computed up to two-loop order in perturbatio
n theory and the 'Ward identity' that relates this tensor to the effec
tive coupling is verified to the same order. We re-examine the renorma
lization group calculation that produced a very accurate numerical val
ue for the effective diffusivity in the rotationally symmetric case an
d formulate two versions based on distinct divisions of the random pot
ential held that gives rise to the flow. Both types of renormalization
group calculation give good results when compared with numerical simu
lations. However, at two-loop order in perturbation theory the two met
hods differ in detail from each other and from the exact perturbation
calculation. This is in contrast to the corresponding results in the i
sotropic case.