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Numerical analysis of subsonic turbulent jets

Başlık çevirisi mevcut değil.

  1. Tez No: 523294
  2. Yazar: MEHMET ONUR ÇETİN
  3. Danışmanlar: Dr. WOLFGANG SCHRÖDER, Dr. PETER JESCHKE
  4. Tez Türü: Doktora
  5. Konular: Makine Mühendisliği, Mechanical Engineering
  6. Anahtar Kelimeler: Belirtilmemiş.
  7. Yıl: 2017
  8. Dil: İngilizce
  9. Üniversite: Rheinisch-Westfälische Technische Hochschule Aachen
  10. Enstitü: Yurtdışı Enstitü
  11. Ana Bilim Dalı: Belirtilmemiş.
  12. Bilim Dalı: Belirtilmemiş.
  13. Sayfa Sayısı: 129

Özet

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Özet (Çeviri)

Noise reduction is one of the major tasks in todays aircraft development and it is also one of the key goals in the European ACARE 2050 targets, which require the perceived noise level of flying aircraft to be reduced by 65 %. The jet development in the near field is strongly influenced by the larger scales of turbulent motions which are in turn affected by the nozzle geometry and the main wing. The prediction of jet noise sources needs detailed knowledge about the unsteady flow field, which can be obtained via highly resolved large eddy simulations (LES). In line with this perspective, this thesis analyzes the impact of nozzle interior details and nozzle exit conditions on the flow and the resulting sound field, and the flow field of a complete nozzle-wing geometry including slat, airfoil, and flap to investigate the sensitivity of flow conditions on the nozzle-wing interaction in the jet near field. First, LES of turbulent axisymmetric hot jets are conducted. Three nozzle geometries of increasing complexity, i.e., a clean nozzle without any built-in components, a centerbody nozzle, and a nozzle with centerbody plus 5 struts are considered to investigate the influence of nozzle interior details on the overall flow and acoustic field. The results evidence that the flow field in the region 35 nozzle radii downstream of the exit is dominated by the flow structures induced by the geometry. Additional nozzle built-in components enhance the turbulent mixing by increasing the turbulent intensity in the jet near field. The centerbody perturbed nozzle configurations reveal a spectral peak in the near nozzle exit region which is caused by the wake flow from the centerbody. Moreover, the centerbody nozzle increases the overall sound pressure level (OASPL) in the near field compared to the clean nozzle and the centerbody-plus-strut nozzle reduces it compared to the centerbody nozzle due to the increased turbulent mixing. It is found that the spectral peak appeared in the flow field analysis also occurs in the acoustic near field. Thereafter, the flow and the acoustic field of two jets are analyzed to determine the impact of exit conditions on the jet development. First, the flow inside the nozzle is part of the overall nozzle-jet analysis such that the turbulent flow at the nozzle exit is determined by the solution of the full discrete conservation equations. This configuration corresponds to the centerbody nozzle solution. Second, the nozzle exit distributions which are used as inflow distributions for the free jet analysis are based on the mean flow profiles plus vortex rings. That is, for the latter case the impact of the nozzle geometry on the jet is not directly taken into account, the nozzle exit distribution is imposed. The flow field analysis shows that the flow field immediately downstream of the nozzle exit is strongly influenced by the flow structures induced by the nozzle geometry. The nozzle included solution possesses an almost 30% higher peak turbulence intensity level which also results in a massively enhanced velocity decay. The peak observed in the centerbody nozzle configuration can not be seen in the nozzle modeled solution since the vortices which generate the peak shedding from centerbody are missing. It is, moreover, found that both jet configurations reveal quite a different qualitative behavior of the sound spectra, especially in the sideline direction where the entropy source term dominates the sound generation. This difference occurs since the noise sources generated by the artificial perturbations are not perfectly mimicked in the nozzle modeled solution. However, the total overall sound pressure level shows the same qualitative behavior for both nozzle configurations. Towards the downstream direction, the sound spectra of both solutions converge. Finally, apart from the conventional isolated nozzle-jet analysis in which there is no flow-solid-body interaction in the free jet field, 3D unsteady flow simulations of a realistic ultra-high bypass-ratio engine and wing are considered to define the influence of various engine conditions on the jet development when there is jet-wing interaction in the free jet region. The Mach number of the wind tunnel is M=0.176, the jet Mach number is M=0.352. Two fan flow conditions are considered where the Mach number of the first setup is M=0.376, and M=0.43 for the second setup. The Reynolds number based on the wind tunnel velocity is Re=150,000. It is found that increasing the fan jet velocity increases the core length of the jet and the turbulence intensity level. Furthermore, spectral analysis in the near jet region suggests that the characteristic frequency of the shear layer instabilities considerably decreases near the wing geometry due to the jet-wing interaction compared to the distributions in the lower side of the jet stream where there is no flow-solid-body interface.

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