全部 标题 作者
关键词 摘要

OALib Journal期刊
ISSN: 2333-9721
费用:99美元

查看量下载量

相关文章

更多...

A LES Study on Passive Mixing in Supersonic Shear Layer Flows Considering Effects of Baffle Configuration

DOI: 10.1155/2014/836146

Full-Text   Cite this paper   Add to My Lib

Abstract:

Under the background of dual combustor ramjet (DCR), a numerical investigation of supersonic mixing layer was launched, focused on the mixing enhancement method of applying baffles with different geometric configurations. Large eddy simulation with high order schemes, containing a fifth-order hybrid WENO compact scheme for the convective flux and sixth-order compact one for the viscous flux, was utilized to numerically study the development of the supersonic mixing layer. The supersonic cavity flow was simulated and the cavity configuration could influence the mixing characteristics, since the impingement process of large scale structures formed inside the cavity could raise the vorticity and promote the mixing. The effect of baffle’s configurations on the mixing process was analyzed by comparing the flow properties, mixing efficiency, and total pressure loss. The baffle could induce large scale vortexes, promote the mixing layer to lose its stability easily, and then lead to the mixing efficiency enhancement. However, the baffle could increase the total pressure loss. The present investigation could provide guidance for applying new passive mixing enhancement methods for the supersonic mixing. 1. Introduction High-speed flight vehicles call for new type propulsion system and scramjet has attracted researchers’ attention to focus on this technique [1]. In order to adapt to the requirements of hypersonic vehicle at different flight Mach numbers, the dual combustor ramjet (DCR) was proposed, which was more superior to the conventional dual mode ramjet. The advantages include without fuel pretreatment, ignition and combustion stability, low Mach number launch, without mode conversion, and so on [2–4]. However, the superiority could result in complexity of the structure of engine and hence complicate internal flow and combustion characteristics. The combustion must occur quickly and requires fuel mix rapidly with oxidizer. In addition, the well mixing of fuel-rich gas from subsonic combustor with supersonic flow could achieve the advantages of DCR, and then the second combustion in supersonic combustor could proceed effectively. However, it is difficult to achieve the fully mixing of high-speed flows. Thus, the mixing enhancement measures to organize stable and efficient combustion in DCR are of importance. The research on the mechanism of mixing layer contributes to perceive the flow stability, transition from laminar to turbulent and turbulence phenomena, finding the factors affecting the mixing efficiency. Initially, the study of the mixing layer was

References

[1]  J. M. Tishkoff, J. P. Drummond, T. Edwards, et al., “Future directions of supersonic combustion research—air force/NASA workshop on supersonic combustion,” AIAA Paper 97-1017, 1997.
[2]  F. S. Billig, P. J. Waltrup, and R. D. Stockbridge, “Integral-rocket dual-combustion ramjets: a new propulsion concept,” Journal of Spacecraft and Rockets, vol. 17, no. 5, pp. 416–724, 1980.
[3]  J. L. Keirsey, “Airbreathing propulsion for defense of the surface fleet,” Johns Hopkins APL Technical Digest, vol. 13, no. 1, pp. 57–68, 1992.
[4]  E. T. Curran, “Scramjet engines: the first forty years,” Journal of Propulsion and Power, vol. 17, no. 6, pp. 1138–1148, 2001.
[5]  D. Papamoschou and A. Roshko, “Compressible turbulent shear layer: an experimental study,” Journal of Fluid Mechanics, vol. 197, pp. 453–477, 1988.
[6]  D. Papamoschou, “Structure of the compressible turbulent shear layer,” AIAA Paper 89-0126, 1989.
[7]  T. L. Jackson and C. E. Grosch, “Inviscid spatial stability of a compressible mixing layer,” Journal of Fluid Mechanics, vol. 208, pp. 609–637, 1989.
[8]  G. S. Elliott and M. Samimy, “Compressibility effects in free shear layers,” Physics of Fluids A, vol. 2, no. 7, pp. 1231–1240, 1990.
[9]  G. S. Elliott, M. Samimy, and S. A. Arnette, “The characteristics and evolution of large-scale structures in compressible mixing layers,” Physics of Fluids, vol. 7, no. 4, pp. 864–876, 1995.
[10]  A. W. Vreman, N. D. Sandham, and K. H. Luo, “Compressible mixing layer growth rate and turbulence characteristics,” Journal of Fluid Mechanics, vol. 320, pp. 235–258, 1996.
[11]  J. B. Freund, S. K. Lele, and P. Moin, “Compressibility effects in a turbulent annular mixing layer. Part 1. Turbulence and growth rate,” Journal of Fluid Mechanics, vol. 421, pp. 229–267, 2000.
[12]  P. Huerre and P. A. Monkewitz, “Absolute and convective instabilities in free shear layers,” Journal of Fluid Mechanics, vol. 159, pp. 151–168, 1985.
[13]  T. L. Jackson and C. E. Grosch, “Absolute/convective instabilities and the convective Mach number in a compressible mixing layer,” Physics of Fluids A, vol. 2, no. 6, pp. 949–954, 1990.
[14]  O. Peroomian and R. E. Kelly, “Absolute and convective instabilities in compressible confined mixing layers,” Physics of Fluids, vol. 6, no. 9, pp. 3192–3194, 1994.
[15]  L.-S. Lee and P. J. Morrist, “Absolute instability in a supersonic shear layer and mixing control,” Journal of Propulsion and Power, vol. 13, no. 6, pp. 763–767, 1997.
[16]  L. P. Bernal and A. Roshko, “Streamwise vortex structure in plane mixing layers,” Journal of Fluid Mechanics, vol. 170, pp. 499–525, 1986.
[17]  G. L. Brown and A. Roshko, “On density effects and large structure in turbulent mixing layers,” Journal of Fluid Mechanics, vol. 64, no. 4, pp. 775–816, 1974.
[18]  H. G?rtler, “On the three-dimensional instability of laminar boundary layers on concave walls,” NACA TM 1375, 1954.
[19]  F. Génin and S. Menon, “Simulation of turbulent mixing behind a strut injector in supersonic flow,” AIAA Journal, vol. 48, no. 3, pp. 526–539, 2010.
[20]  N. A. Adams and K. Shariff, “A high-resolution hybrid compact-eno scheme for shock-turbulence interaction problems,” Journal of Computational Physics, vol. 127, no. 1, pp. 27–51, 1996.
[21]  S. Pirozzoli, “Conservative hybrid compact-WENO schemes for shock-turbulence interaction,” Journal of Computational Physics, vol. 178, no. 1, pp. 81–117, 2002.
[22]  E. J. Gutmark, K. C. Schadow, and K. H. Yu, “Mixing enhancement in supersonic free shear flows,” Annual Review of Fluid Mechanics, vol. 27, no. 1, pp. 375–417, 1995.
[23]  D. M. Bushnell, “Hypervelocity scramjet mixing enhancement,” Journal of Propulsion and Power, vol. 11, no. 5, pp. 1088–1090, 1995.
[24]  J. M. Seiner, S. M. Dash, and D. C. Kenzakowski, “Historical survey on enhanced mixing in scramjet engines,” Journal of Propulsion and Power, vol. 17, no. 6, pp. 1273–1286, 2001.
[25]  V. A. Vinogradov, Y. M. Shikhman, and C. Segal, “A review of fuel pre-injection in supersonic, chemically reacting flows,” Applied Mechanics Reviews, vol. 60, no. 1–6, pp. 139–148, 2007.
[26]  S. Sujith, T. M. Muruganandam, and J. Kurian, “Effect of trailing ramp angles in strut-based injection in supersonic flow,” Journal of Propulsion and Power, vol. 29, no. 1, pp. 66–78, 2013.
[27]  P. Behrouzi and J. J. McGuirk, “Effect of tabs on rectangular jet plume development,” Journal of Propulsion and Power, vol. 25, no. 4, pp. 930–939, 2009.
[28]  D. P. Mishra and K. V. Sridhar, “Numerical study of effect of fuel injection angle on the performance of a 2D supersonic cavity combustor,” Journal of Aerospace Engineering, vol. 25, no. 2, pp. 161–167, 2012.
[29]  E. M. Fernando and S. Menon, “Mixing enhancement in compressible mixing layers: an experimental study,” AIAA Journal, vol. 31, no. 2, pp. 278–285, 1993.
[30]  T. Sunami, M. N. Wendt, and M. Nishioka, “Supersonic mixing and combustion control using streamwise vortices,” AIAA Paper 98-3271, 1998.
[31]  C. J. Bourdon and J. C. Dutton, “Mixing enhancement in compressible base flows via generation of streamwise vorticity,” AIAA Journal, vol. 39, no. 8, pp. 1633–1635, 2001.
[32]  M. Kodera, T. Sunami, and F. Scheel, “Numerical study on the supersonic mixing enhancement using streamwise vortices,” AIAA Paper 2002-5117, 2002.
[33]  S. Watanabe and M. G. Mungal, “Velocity fields in mixing-enhanced compressible shear layers,” Journal of Fluid Mechanics, vol. 522, pp. 141–177, 2005.
[34]  N. Chauvet, S. Deck, and L. Jacquin, “Numerical study of mixing enhancement in a supersonic round jet,” AIAA Journal, vol. 45, no. 7, pp. 1675–1687, 2007.
[35]  S. Sujith, T. M. Muruganandam, and J. Kurian, “Effect of trailing ramp angles in strut-based injection in supersonic flow,” Journal of Propulsion and Power, vol. 29, no. 1, pp. 66–78, 2013.
[36]  S. G. Goebel, J. C. Dutton, H. Krier, and J. P. Renie, “Mean and turbulent velocity measurements of supersonic mixing layers,” Experiments in Fluids, vol. 8, no. 5, pp. 263–272, 1990.
[37]  P. J. Lu and K. C. Wu, “On the shock enhancement of confined supersonic mixing flows,” Physics of Fluids A, vol. 3, no. 12, pp. 3046–3062, 1991.
[38]  Y.-X. Ren, M. Liu, and H. Zhang, “A characteristic-wise hybrid compact-WENO scheme for solving hyperbolic conservation laws,” Journal of Computational Physics, vol. 192, no. 2, pp. 365–386, 2003.
[39]  C. S. Peskin, “Flow patterns around heart valves: a numerical method,” Journal of Computational Physics, vol. 10, no. 2, pp. 252–271, 1972.

Full-Text

comments powered by Disqus

Contact Us

service@oalib.com

QQ:3279437679

WhatsApp +8615387084133

WeChat 1538708413