The steady flow of a power-law (Ostwald) fluid between two differentia
lly rotating, parallel, co-axial discs has been considered for both la
rge and small Reynolds number. All edge effects of the discs are negle
cted, the discs rotate in the same sense and the distance between the
two discs is much smaller than their radius. In the large Reynolds num
ber case a similarity solution is sought. It is assumed that the flow
consists of boundary layers on the discs, while the core rotates as a
rigid body with speed intermediate of those of the discs. The boundary
layer is thinner than in the equivalent Newtonian problem, and the de
cay of the boundary layers is found to be algebraic. This slow decay c
ontrasts with the faster exponential decay in the Newtonian case. For
the low Reynolds number problem, the ratio of the disc separation to r
adius was taken to be much smaller than the Reynolds number. This is,
in effect, a lubrication-type problem. The velocity components are exp
ressed as expansions in ascending powers of the Reynolds number. For b
oth the large and small Reynolds number flow, the torque is calculated
as a function of the disc speeds, for various values of the power-law
index n.