Influence of the Reynolds number on the instant flow evolution of a turbulent rectangular free jet of air. Average Particle Image Velocimetry (PIV) visualizations and measurements
The paper is aimed at investigating the influence of the Reynolds number on the instant flow evolution of
a rectangular free jet of air in the range of Reynolds numbers from Re = 35,300 to Re = 2,200, where the
Reynolds number, Re, is defined according to the hydraulic diameter, D, of a rectangular slot of height H,
equal to about D = 2H. The Particle Image Velocimetry (PIV) technique allows obtaining the instant PIV
visualizations on the central symmetry section of the rectangular jet. The visual inspection of the instant
frames with one and two vortices, except for Re = 35,300 where only one vortex images are detected,
shows that after the jet exit is present the Flow with Constant Instant Height, with a length LCIH which
increases with the decrease of the Reynolds number, from a ratio LCIH/H equal to LCIH/H = 0.9 at
Re = 35,300 to LCIH/H = 4.0 at Re = 2,200. The instant PIV measurements, carried out at several distances
from the jet exit, show that the variations of the ratio U=U0 of the centerline instant velocity, U, to the
exit average velocity, U0, remain below ±4% for a length LCIV, defining the Flow with Constant Instant
Velocity on the centerline. The ratio LCIV/H increases from LCIV/H = 1.1 at Re = 35,300 to LCIV/H = 4.1 at
Re = 2,200 and is quite similar to LCIH/H. The instant PIV measurements of the centerline turbulence intensity,
Tu, show that its variations remain below ±4% for a length LCIT, defining the Flow with Constant
Instant Turbulence on the centerline. The ratio LCIT/H is equal to LCIV/H. The instant PIV velocity profiles
in the transverse direction, are practically unchanged for a length LUVP which defines the flow with
Unchanged Velocity Profile. The four lengths LUVP = LCIH = LCIV = LCIT are considered equal, defining the
Flow with Negligible Disturbances, with length LND, or first type of flow, L1, which is in agreement with
the average length of the flow with Constant Height, LCH, in the turbulent and laminar regime, and with
the average length of the Undisturbed flow, LU, in the turbulent regime. The instant PIV frames show the
presence, after the flow with negligible disturbances, of the Flow with Small Variations of the Height,
where the jet height varies slightly without forming the vortex. The length of the flow with Small Variation
of the Height is LSVH, and the first vortex appears after the total length (LND + LSVH). The variations of
the instant PIV measurements of the centerline turbulence intensity, Tu, increase after the length LCIT, but
remaining below ±5–9% for a length LSVT, which defines the Flow with Small Variation of the Turbulence.
The total length (LCIT + LSVT) is comparable to (LCIH + LSVH) in the turbulent and laminar regimes, and can be
assumed equal to the sum of the lengths of the flows with negligible and small disturbances, LND + LSD = L2,
which is in agreement with the average length of the undisturbed flow, LU, in the laminar regime. The
instant PIV frames show the flow with Coherent Vortices after L2, with a length LCV, followed by the
vortices breakdown. The instant PIV frames allow visualizing the end of the flow with Coherent Vortices,
defining the total length of the flows with negligible and small disturbances, and coherent vortices, as
LND + LSD + LCV = L3, which is in good agreement with the average length of the potential core, LP