We excite an epicyclic motion, the amplitude of which depends on the vertic
al position, z, in a simulation of a turbulent accretion disc. An epicyclic
motion of this kind may be caused by a warping of the disc. By studying ho
w the epicyclic motion decays, we can obtain information about the interact
ion between the warp and the disc turbulence. A high-amplitude epicyclic mo
tion decays first by exciting inertial waves through a parametric instabili
ty, but its subsequent exponential damping may be reproduced by a turbulent
viscosity. We estimate the effective viscosity parameter, alpha(v), pertai
ning to such a vertical shear. We also gain new information on the properti
es of the disc turbulence in general, and measure the usual viscosity param
eter, alpha(h), pertaining to a horizontal (Keplerian) shear. We find that,
as is often assumed in theoretical studies, alpha(v) is approximately equa
l to alpha(h) and both are much less than unity, for the field strengths ac
hieved in our local box calculations of turbulence. In view of the smallnes
s (similar to 0.01) of alpha(v) and alpha(h) we conclude that for beta = p(
gas)/p(mag) similar to 10 the time-scale for diffusion or damping of a warp
is much shorter than the usual viscous time-scale. Finally, we review the
astrophysical implications.