Instantaneous, dynamic and time-averaged characteristics of the vortex stru
ctures which are shed from the dimples placed on one wall of a channel are
described. The dimpled test surface contains 13 staggered rows of dimples i
n the streamwise direction, where each dimple has a print diameter of 5.08
cm, and a ratio of depth to print diameter of 0.2. Considered are Reynolds
numbers (based on channel height) Re-H from 600 to 11 000, and ratios of ch
annel height to dimple print diameter H/D of 0.25, 0.50, and 1.00. For all
three H/D, a primary vortex pair is periodically shed from the central port
ion of each dimple, including a large upwash region. This shedding occurs p
eriodically and continuously, and is followed by inflow advection into the
dimple cavity. The frequency of these events appears to scale on time-avera
ged bulk velocity and dimple print diameter, which gives nondimensional fre
quencies of 2.2-3.0 for all three H/D values considered. As H/D decreases,
(i) the strength of the primary vortex pair increases, and (ii) two additio
nal secondary vortex pairs (which form near the spanwise edges of each dimp
le) become significantly stronger, larger in cross section, and more appare
nt in flow visualization images and in surveys of time-averaged, streamwise
vorticity. The locations of these primary and secondary vortex pairs near
the dimpled surface coincide closely with locations where normalized Reynol
ds normal stress is augmented. This evidences an important connection betwe
en the vortices, Reynolds normal stress, and mixing. The large-scale unstea
diness associated with this mixing is then more pronounced, and encompasses
larger portions of the vortex structure (and thus extends over larger volu
mes) as H/D increases from 0.25 to 1.0. (C) 2001 American Institute of Phys
ics.