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Unsteady pulsating flowfield over spiked axisymmetric forebody at hypersonic flows
Date Issued
01-01-2022
Author(s)
Sugarno, Mohammed Ibrahim
Indian Institute of Technology, Madras
Karthick, S. K.
Jagadeesh, Gopalan
Abstract
The paper gives experimental observations of the hypersonic flow past an axisymmetric flat-face cylinder with a protruding sharp-tip spike. Unsteady pressure measurements and high-speed schlieren images are performed in tandem on a hypersonic Ludwieg tunnel at a freestream Mach number of M ∞ = 8.16 at two different freestream Reynolds numbers based on the base body diameter (R e D = 0.76 × 10 6 and 3.05 × 10 6). The obtained high-speed images are subjected further to modal analysis to understand the flow dynamics parallel to the unsteady pressure measurements. The protruding spike of length to base body diameter ratio of [l / D] = 1 creates a familiar form of an unsteady flowfield called "pulsation."Pressure loading and fluctuation intensity at two different ReD cases are calculated. A maximum drop of 98.24% in the pressure loading and fluctuation intensity is observed between the high and low ReD cases. Due to the low-density field at low ReD case, almost all image analyses are done with the high ReD case. Based on the analysis, a difference in the pulsation characteristics is noticed, which arises from two vortical zones, each from a system of two "λ"shocks formed during the "collapse"phase ahead of the base body. The interaction of shedding vortices from the λ-shocks' triple-points, along with the rotating stationary waves, contributes to the asymmetric high-pressure loading and the observation of shock pulsation on the flat-face cylinder. The vortical interactions forming the second dominant spatial mode with a temporal mode carry a dimensionless frequency (f 2 D / u ∞ ≈ 0.34) almost twice that of the fundamental frequency (f 1 D / u ∞ ≈ 0.17). The observed frequencies are invariant irrespective of the ReD cases. However, for the high-frequency range, the spectral pressure decay is observed to follow an inverse and -7/3 law for the low and high ReD cases, respectively.
Volume
34