This paper considers the creeping flows generated by a disk moving edg
ewise parallel to a rigid wall or free surface, a disk oscillating edg
ewise in unbounded fluid and a hole in the rigid plane that bounds a s
hear flow excited by a parallel moving plane. The analyses for the thr
ee cases follow a similar pattern and several simplifying strategies a
re introduced to obtain significant improvements on the presentations
suggested by previous work on such flows. Indeed, the resulting integr
al equations for the first disk problem are similar to those solved fo
r the corresponding broadside motion. The drag force is shown to slowl
y approach its limit value as the disk is placed nearer to the free su
rface. The oscillatory hydrodynamic force is shown to have only Stokes
and Basset components. The error in previously assuming the shear flo
w to extend to infinity is shown to be of order H-3, where H is the se
paration distance between the bounding planes.