2013
DOI: 10.1007/s12567-013-0045-6
|View full text |Cite
|
Sign up to set email alerts
|

Investigation of the turbulent wake flow of generic launcher configurations via a zonal RANS/LES method

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

1
13
0

Year Published

2014
2014
2024
2024

Publication Types

Select...
3
2
1

Relationship

2
4

Authors

Journals

citations
Cited by 11 publications
(14 citation statements)
references
References 21 publications
1
13
0
Order By: Relevance
“…Statnikov et al [13] showed that the strength of the recompression shocks and expansion waves directly depends on the de §ection of the shedding shear layer which is determined by the tail geometry and, possibly, other geometrical obstacles, e. g., a strongly aftexpanding jet plume that emanates from the nozzle in real §ight conditions. For the blunt-base and nozzle-dummy con¦gurations, the large expansion angles β e of the shedding shear layer shown in Fig.…”
Section: Spatial Wall Pressure Distributionmentioning
confidence: 99%
See 2 more Smart Citations
“…Statnikov et al [13] showed that the strength of the recompression shocks and expansion waves directly depends on the de §ection of the shedding shear layer which is determined by the tail geometry and, possibly, other geometrical obstacles, e. g., a strongly aftexpanding jet plume that emanates from the nozzle in real §ight conditions. For the blunt-base and nozzle-dummy con¦gurations, the large expansion angles β e of the shedding shear layer shown in Fig.…”
Section: Spatial Wall Pressure Distributionmentioning
confidence: 99%
“…14b, the pressure §uctuations inside the shed shear layer (region (ii) in Fig. 14a) feature a sharp peak at a distinct dominant frequency of about Sr D = 0.2 that appears due to the vortex shedding at the model shoulder [33] and originally Figure 16 Comparison of the numerical RANS/LES (dashed curves) and experimental (solid curves) pressure spectra on the base wall (extracted from [13]) at ϕ = 180 • and r = 40 mm (t = 1200 · 50D/U∞): 1 ¡ blunt base; and 2 ¡ nozzle dummy is not present in the incoming boundary layer. The latter possesses a broadband spectrum without any distinct dominant frequencies over a wide range of Strouhal numbers, as illustrated by curve 1 in Fig.…”
Section: Analysis Of the Dynamic Wake Flow Behaviormentioning
confidence: 99%
See 1 more Smart Citation
“…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: 73%
“…DNS is still restricted to low Reynolds numbers and a small integration domain. In contrast, LES (Meliga et al [16]) and particularly hybrid approaches like DES (Deck and Thorigny [17]) and zonal RANS/LES (Statnikov et al [18]) allow time-resolved computation of the dynamic wake flow field at practically relevant Reynolds-numbers and were found to be a good compromise between costs and accuracy for computation of the wake flow of space launchers.…”
mentioning
confidence: 99%