$\require{mediawiki-texvc}$

연합인증

연합인증 가입 기관의 연구자들은 소속기관의 인증정보(ID와 암호)를 이용해 다른 대학, 연구기관, 서비스 공급자의 다양한 온라인 자원과 연구 데이터를 이용할 수 있습니다.

이는 여행자가 자국에서 발행 받은 여권으로 세계 각국을 자유롭게 여행할 수 있는 것과 같습니다.

연합인증으로 이용이 가능한 서비스는 NTIS, DataON, Edison, Kafe, Webinar 등이 있습니다.

한번의 인증절차만으로 연합인증 가입 서비스에 추가 로그인 없이 이용이 가능합니다.

다만, 연합인증을 위해서는 최초 1회만 인증 절차가 필요합니다. (회원이 아닐 경우 회원 가입이 필요합니다.)

연합인증 절차는 다음과 같습니다.

최초이용시에는
ScienceON에 로그인 → 연합인증 서비스 접속 → 로그인 (본인 확인 또는 회원가입) → 서비스 이용

그 이후에는
ScienceON 로그인 → 연합인증 서비스 접속 → 서비스 이용

연합인증을 활용하시면 KISTI가 제공하는 다양한 서비스를 편리하게 이용하실 수 있습니다.

Computational Investigation of Turbulent Swirling Flows in Gas Turbine Combustors 원문보기

International journal of fluid machinery and systems, v.1 no.1, 2008년, pp.1 - 9  

Benim, A.C. (Department of Mechanical and Process Engineering, Duesseldorf University of Applied Sciences) ,  Escudier, M.P. (Department of Engineering, University of Liverpool) ,  Stopford, P.J. (ANSYS Europe Ltd.) ,  Buchanan, E. (Combustor Development, Siemens Industrial Turbomachinery Ltd.) ,  Syed, K.J. (Combustor Development, Siemens Industrial Turbomachinery Ltd.)

Abstract AI-Helper 아이콘AI-Helper

In the first part of the paper, Computational Fluid Dynamics analysis of the combusting flow within a high-swirl lean premixed gas turbine combustor and over the $1^{st}$ row nozzle guide vanes is presented. In this analysis, the focus of the investigation is the fluid dynamics at the com...

주제어

AI 본문요약
AI-Helper 아이콘 AI-Helper

* AI 자동 식별 결과로 적합하지 않은 문장이 있을 수 있으니, 이용에 유의하시기 바랍니다.

제안 방법

  • The solution domain is defined to start in the annular channel, slightly upstream of the combustor. Preliminary 3D RANS computations were performed for a domain covering the guide vanes of the swirl generator and the axial inlet channel. In the main computations, the block-structured grid with conformal block interfaces consisted of approximately 600,000 hexa cells.
  • The solution domain is defined to include the combustor and the swirl generator. Preliminary 3D RANS computations were performed for a domain covering the plenum and channels of the swirl generator to obtain the inlet conditions. For the main computations, the block-structured grid consisted of approximately 1,000,000 hexahedral finite volumes.
  • The experimental data shows a forced-vortex-like region in the vicinity of the axis, changing over to a free-vortex-like distribution at higher values of the radial coordinate. It is interesting to note that the vortex core first radially expands between the stations x=10mm and x=50mm, and then contracts between x=50mm and x=160mm.
  • Although many analytical and numerical investigations have been conducted to address vortex breakdown and the criticality of the vortex core [3-6] much of this work is based upon simplifying assumptions, such as axisymmetry in conjunction with a Reynolds Averaged Navier-Stokes (RANS) based turbulence modelling. These studies have revealed much about the behaviour of vortical flows but they fall short of delivering quantitative information that can be used in the design of combustors, since low- frequency transient motion of coherent structures, which can play a very important role in swirling flows, cannot be represented adequately by a RANS based turbulence modelling approach.

대상 데이터

  • Preliminary 3D RANS computations were performed for a domain covering the plenum and channels of the swirl generator to obtain the inlet conditions. For the main computations, the block-structured grid consisted of approximately 1,000,000 hexahedral finite volumes.
  • Preliminary 3D RANS computations were performed for a domain covering the guide vanes of the swirl generator and the axial inlet channel. In the main computations, the block-structured grid with conformal block interfaces consisted of approximately 600,000 hexa cells.
  • The experimental results show recirculation regions as well as on the axis, and in the corner downstream of the sudden expansion into the combustor, at the axial stations x=10mm and x=50mm. At x=160mm, it can be observed that both recirculation zones have disappeared, and, on the axis, the reverse flow zone is replaced by a strong jet-like overshoot.

이론/모형

  • Although many analytical and numerical investigations have been conducted to address vortex breakdown and the criticality of the vortex core [3-6] much of this work is based upon simplifying assumptions, such as axisymmetry in conjunction with a Reynolds Averaged Navier-Stokes (RANS) based turbulence modelling. These studies have revealed much about the behaviour of vortical flows but they fall short of delivering quantitative information that can be used in the design of combustors, since low- frequency transient motion of coherent structures, which can play a very important role in swirling flows, cannot be represented adequately by a RANS based turbulence modelling approach.
  • In the first part of the paper, it is demonstrated that very encouraging results can indeed be obtained for a high-swirl lean premixed gas turbine combustor flow, which qualitatively agree with the measurements [7], applying an Unsteady RANS (URANS) based turbulence modelling approach, utilizing a Reynolds Stress Model (RSM) as the statistical turbulence model.
  • DES: Detached Eddy Simulations [15,16], as a LES-RANS hybrid modelling approach. In the present application, the model is based on the Shear Stress Transport (SST) model of Menter [17] as the background RANS model.
  • The rig operates at Re=7000 (Reynolds number is based on the diameter and the bulk axial velocity of the combustor). Measurements were performed by Laser Doppler Anemometry (LDA). Different swirl levels were obtained by adjusting the swirler guide vanes angles.
  • The analysis has been based on the commercial general-purpose CFD software ANSYS-CFX [8]. It is already known [9] that certain Reynolds stress components are significantly modified due to the action of flow curvature and pressure gradient within swirling flows.
본문요약 정보가 도움이 되었나요?

참고문헌 (23)

  1. Cramb, D. J. and McMillan, R., 2001, “Tempest Dual Fuel DLE Development and Commercial Operating Experience andUltra Low NOx Gas Operation”, ASME Paper 2001-GT-76. 

  2. Escudier, M. and Keller, J. J., 1983, “Vortex Breakdown: A Two Stage Transition”, Aerodynamics of Vortical Type Flows inThree Dimensions”, AGARD CP No. 342, Paper No. 25. 

  3. Weber, R., Boysan, F., Swithenbank, J. and Roberts, P. A., 1986, “Computation of Near Field Aerodynamics of SwirlingExpanding Flows’, Proc. 21st Symp. (Int.) Combustion, The Combustion Institute, Pittsburgh, pp. 1435-1443. 

  4. Hogg, S. and Leschziner, 1988, “Computation of Highly Swirling Confined Flow with a Reynolds Stress Turbulence Model’,AIAA Journal, Vol. 27, pp. 57-63. 

  5. Benim, A. C., 1990, “Finite Element Analysis of Confined Swirling Flows”, International Journal for Numerical Methods in Fluids, Vol. 11, pp. 697-717. 

  6. Spall, R. E. and Gatski, T. B., 1995, “Numerical Calculations of 3D Turbulent Vortex Breakdown”, International Journal forNumerical Methods in Fluids, Vol. 20, pp. 307-318. 

  7. Turrell, M. D., Stopford, P. J., Syed, K. J. and Buchanan, E., 2004, “CFD Simulation of the Flow within and Downstream of aHigh-Swirl Lean Premixed Gas Turbine Combustor”, ASME Paper GT2004-53112. 

  8. ANSYS-CFX-10, 2006, “SolverManual”, ANSYS Inc. 

  9. Sloan, D. G., Smith, P. J. and Smoot, L. D., 1986, “Modelling of Swirl in Turbulent Flow Systems”, Progress in Energy andCombustion Science, Vol. 12, pp. 163-250. 

  10. Launder, B. E., Reece, G. J. and Rodi, W., 1975, “Progress in the Development of a Reynolds-Stress Turbulence Closure”,Journal of Fluid Mechanics, Vol. 68, pp. 537-566. 

  11. Speziale, C. G., Sarkar S. and Gatski, T. B., 1991, “Modelling the Pressure-Strain Correlation of Turbulence”, Journal ofFluid Mechanics, Vol. 227, pp. 245-272. 

  12. Sagaut, P., 2002, Large Eddy Simulation for Incompressible Flows ? An Introduction, 2nd Ed., Springer, Berlin. 

  13. Smagorinsky, J., 1963, “General Circulation Experiments With the Primitive Equations. I: The Basic Experiment”. MonthlyWeather Review, Vol. 91, pp. 99-164. 

  14. Hinze, J. O., 1959, Turbulence, McGraw-Hill, New York. 

  15. Travin, A., Shur, M., Strelets, M. and Spalart, P., 1999, “Detached-Eddy Simulations Past a Circular Cylinder”, Flow,Turbulence and Combustion, Vol. 63, pp. 293-313. 

  16. Strelets, M., 2001, “Detached Eddy Simulation of Massively Separated Flows”, AIAA Paper 2001-0879. 

  17. Menter, F. R., 1994, “Two Equation Eddy-Viscosity Turbulence Models for Engineering Applications”, AIAA Journal, Vol.32, pp. 1598-1695. 

  18. Magnussen, B. and Hjertager, B., 1976, “On Mathematical Modelling of Turbulent Combustion with Special Emphasis on Soot Formation and Combustion”, Proc. 16th Symp. (Int.) Combustion, The Combustion Institute, Pittsburgh, pp. 719-729. 

  19. Westbrook, C. and Dryer, H., 1981, “Simplified Reaction Mechanisms for the Oxidation of Hydrocarbon Fuels in Flames”, Combustion Science and Technology, Vol. 2, pp. 31-47. 

  20. Bradshaw, P. (Ed.), 1978, Turbulence, Springer, Berlin. 

  21. Peyret, R (Ed.), 2000, Handbook of Computational Fluid Mechanics, Academic Press, San Diego. 

  22. Escudier, M. P. and Keller, J. J., 1985, “Recirculation in Swirling Flow: A Manifestation of Vortex Breakdown”, AIAAJournal, Vol. 23, pp. 111-116. 

  23. Escudier, M. P., Bornstein, J. and Zehnder, N., 1980, “Observations and LDA Measurements of Confined Turbulent Vortex Flow”, Journal of Fluid Mechanics, Vol. 98, pp. 490-463. 

관련 콘텐츠

오픈액세스(OA) 유형

GOLD

오픈액세스 학술지에 출판된 논문

섹션별 컨텐츠 바로가기

AI-Helper ※ AI-Helper는 오픈소스 모델을 사용합니다.

AI-Helper 아이콘
AI-Helper
안녕하세요, AI-Helper입니다. 좌측 "선택된 텍스트"에서 텍스트를 선택하여 요약, 번역, 용어설명을 실행하세요.
※ AI-Helper는 부적절한 답변을 할 수 있습니다.

선택된 텍스트

맨위로