The velocity fluctuations experimentally detected in the wake of a prism ha-
ving triangular cross-section and an aspect ratio H/w = 3.0 are characterized. It
is shown that, besides the fluctuations induced by an alternate vortex shedding
with Strouhal number St ≈ 0.16, further components are present, with different
relative intensities in different wake regions. A spectral contribution at St ≈ 0.05
is found to dominate all the velocity signals in the upper-wake and it is attributed
to a vertical, in-phase oscillation of a couple of counter-rotating axial vortices de-
taching from the front edges of the model free-end. An intermediate component
is also ascertained occurring at St ≈ 0.09. The analysis of a previously available
LES simulation was fundamental for the interpretation of the physical mechanism
giving rise to this flow fluctuation, which is associated with the oscillations of a
transversal shear layer detaching from the rear edge of the model free-end. Pro-
ceeding downstream it bends downwards into the wake in such a way to be reversed
upstream impinging the rear surface of the model. Consequently, a recirculation
region is delimited by this transversal shear layer. This feature is also assessed
from the pressure measurements carried out on the model surfaces; indeed, a pres-
sure maximum was ascertained on the rear surface at z/H = 1/3 and fluctuations
at St ≈ 0.09 are singled out just at the locations below the recirculation region.
Furthermore, the statistics of this frequency are comparable to the ones related to
the same spectral component singled out in proximity to rear edge of the free-end,
and thus most probably are generated from the same vorticity structure, viz. the
transversal shear layer. From the numerical visualizations of the vorticity field it
is observed that the fluctuations of the recirculation region are strictly connected
with the vortex shedding. Lateral vorticity sheets are dragged in the upper wake
generating in correspondence to the wake symmetry plane a vertical \action" on
the transversal shear layer directly. Most probably this intricate wake morphology
is the physical mechanism giving rise to the oscillations of the recirculation region.
Furthermore, it is experimentally assessed that modifications on the vertical edges
of the model generate a variation of the vortex shedding frequency comparable to
the one produced on the fluctuation frequency of the transversal shear layer. Howe-
ver, no variations were found in the fluctuations at the lower frequency in the upper
part of the wake, which suggests that they are likely to be essentially connected
with an instability of the axial vortices originating from the free-end