UFR 3-32 Evaluation: Difference between revisions
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region. The agreement with the experiment is also generally satisfactory | region. The agreement with the experiment is also generally satisfactory | ||
for the Reynolds shear stress. | for the Reynolds shear stress. | ||
Longitudinal evolution of turbulence spectra in the spanwise direction | |||
are presented in Figure 7 for both large and narrow span simulations. In | |||
the separation region, it appears that a large part of the energy is | |||
contained in the small wave numbers in the large span computation. The | |||
cutoff wave number imposed by the finite span is too large in the narrow | |||
span simulation. This forces the energy to concentrate at smaller scale and | |||
affects the results. | |||
Low frequency movements of the reflected shock are clearly observed in | |||
Figure 8. As in the experiment the frequency of the power spectral density | |||
maximum is located at St=0.03. The agreement on the energy distribution | |||
between the narrow span computation and the experiment is very good. | |||
<br/> | <br/> | ||
Revision as of 09:09, 12 August 2013
Planar shock-wave boundary-layer interaction
Semi-confined Flows
Underlying Flow Regime 3-32
Evaluation
Comparison of CFD Calculations with Experiments
LES versus experiment at shock generator angle of 8 degrees
Velocity fluctuations in a plane parallel to the wall evidence the presence of low and high velocity streaks that populates canonical boundary layers. After the separation (identified by the first dashed line), the size of turbulent structures in the spanwise direction significantly increases and further downstream the turbulence slowly relaxes toward its canonical state. This figure illustrates the fact that the simulation is capable of capturing most of the finest turbulent structures present in a supersonic boundary layer.
Quantitative comparisons in the symmetry plane are shown in Figure 6. The agreement between experiment and simulation is very good in the symmetry plane for the longitudinal velocity except in the separation bubble region. Nevertheless, it is important to mention that this region is very sensitive to the nature of inflow perturbations since a large variability of the results in this area has already been observed in the experiment, the 2006 data differing from the 2007 one, specifically in this region. The agreement with the experiment is also generally satisfactory for the Reynolds shear stress.
Longitudinal evolution of turbulence spectra in the spanwise direction are presented in Figure 7 for both large and narrow span simulations. In the separation region, it appears that a large part of the energy is contained in the small wave numbers in the large span computation. The cutoff wave number imposed by the finite span is too large in the narrow span simulation. This forces the energy to concentrate at smaller scale and affects the results.
Low frequency movements of the reflected shock are clearly observed in Figure 8. As in the experiment the frequency of the power spectral density maximum is located at St=0.03. The agreement on the energy distribution between the narrow span computation and the experiment is very good.
Contributed by: Jean-Paul Dussauge — Orange
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