The effect of turbulent
wind-tunnel-wall boundary
layers on density change measurements obtained with focused laser
differential interferometry (FLDI) was studied using a detailed direct
numerical simulation (DNS) of the wall from the Boeing/AFOSR Mach-6
Quiet Tunnel run in its noisy configuration. The DNS was probed with
an FLDI model that is capable of reading in three-dimensional
time-varying density fields and computing the FLDI response. Simulated
FLDI measurements smooth the boundary-layer root-mean-square (RMS)
profile relative to true values obtained by directly extracting the
data from the DNS. The peak of the density change RMS measured by the
FLDI falls within 20% of the true density change RMS. A relationship
between local spatial density change and temporal density fluctuations
was determined and successfully used to estimate density fluctuations
from the FLDI measurements. FLDI measurements of the freestream
fluctuations are found to be dominated by the off-axis tunnel-wall
boundary layers for lower frequencies despite spatial suppression
provided by the technique. However, low-amplitude (0.05%–5% of the
mean density) target signals placed along the tunnel centerline were
successfully measured over the noise of the boundary layers (which
have RMS values of about 12% of the mean). Overall, FLDI was shown to
be a useful technique for making quantitative turbulence measurements
and to measure finite-width sinusoidal signals through turbulent
boundary layers, but may not provide enough off-focus suppression to
provide accurate freestream noise measurements, particularly at lower
frequencies.
Femtosecond laser electronic excitation tagging (FLEET) velocimetry was used in the boundary layer of an ogive-cylinder model in a Mach-6 Ludwieg tube. One-dimensional velocity profiles were extracted from the FLEET signal in laminar boundary layers from pure
N
2
flows at unit Reynolds numbers ranging from
3.4
×
10
6
/
m
to
3.9
×
10
6
/
m
. The effects of model tip bluntness and the unit Reynolds number on the velocity profiles were investigated. The challenges and strategies of applying FLEET for direct boundary layer velocity measurement are discussed. The potential of utilizing FLEET velocimetry for understanding the dynamics of laminar and turbulent boundary layers in hypersonic flows is demonstrated.
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