Progress in Flight Physics 2013
DOI: 10.1051/eucass/201305209
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Investigations on the turbulent wake of a generic space launcher geometry in the hypersonic flow regime

Abstract: The turbulent wake §ow of generic rocket con¦gurations is investigated experimentally and numerically at a freestream Mach number of 6.0 and a unit Reynolds number of 10 · 10 6 m −1 . The §ow condition is based on the trajectory of Ariane V-like launcher at an altitude of 50 km, which is used as the baseline to address the overarching tasks of wake §ows in the hypersonic regime like §uid-structural coupling, reverse hot jets and base heating. Experimental results using pressure transducers and the high-speed S… Show more

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Cited by 18 publications
(18 citation statements)
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“…16. Additionally, the numerical and experimental base pressure spectra feature also clearly pronounced peaks in the range of Sr D ≈ 0.05 which are presumably associated with the oscillatory movement of the large-scale toroidal vortex within the separation bubble as known from the former investigations performed by the authors on a similar generic con¦guration [34].…”
Section: Analysis Of the Dynamic Wake Flow Behaviorsupporting
confidence: 57%
“…16. Additionally, the numerical and experimental base pressure spectra feature also clearly pronounced peaks in the range of Sr D ≈ 0.05 which are presumably associated with the oscillatory movement of the large-scale toroidal vortex within the separation bubble as known from the former investigations performed by the authors on a similar generic con¦guration [34].…”
Section: Analysis Of the Dynamic Wake Flow Behaviorsupporting
confidence: 57%
“…13 to reveal dynamic e¨ects of the recirculation zone on the rocket structure at supersonic §ow conditions. In the radial direction, the time averaged base pressure coe©cient remains at the constant level of c p ≈ −0.03, whereas its rms value exhibits a distinct peak (c p rms ≈ 0.00045) at the inner base corner at x/D ≈ 0.205 which can be explained by high dynamic motion of a large scale toroidal secondary vortex described in [17]. In the streamwise direction, the mean pressure coe©cient remains nearly constant up to x/D ≈ 0.5 where the recompression shock occurs and subsequently, an increase in c p takes place.…”
Section: Supersonic Wake Flowmentioning
confidence: 93%
“…Each unshaped §ow circulation downstream of the base leads to a small shift in the position of the recompression shock and vice versa. The distinct mode of the recompression shock oscillations was determined experimentally and numerically in the range of Sr D ≈ 0.18 [17]. The observed fourth corresponding mode in the base pressure spectra Sr D = 0.192 at r/D = 0.46 is assumed to be a footprint of this coupled e¨ect.…”
Section: Supersonic Wake Flowmentioning
confidence: 98%
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“…As shown by Statnikov et al [18][19][20] for both transonic and supersonic cases, numerical results such as computed flow field topology, time-averages and fluctuations of base pressure signals as well as its spectra satisfactorily agree with the experimental data from literature and experimental investigations conducted within TRR 40 [21][22][23]. Using classical spectral analysis and correlation methods, several distinct frequencies were identified indicating a periodic behavior of the base-flow dynamics, e.g., Sr D D 0:1 (shear layer flapping), Sr D D 0:2 (von Kármán vortex shedding) as well as a number of dominant peaks at lower (Sr D 0:05/ and considerably higher frequencies (Sr D 0:7 and Sr D 1) with not fully understood origins.…”
mentioning
confidence: 82%