This study concerns a 2.5 pressure ratio centrifugal compressor stage consisting of a splittered unshrouded impeller and a vaned diffuser. The aim of this paper is to investigate the modifications of the flow structure when the operating point moves from peak efficiency to near stall. The investigations are based on the results of unsteady three-dimensional simulations, in a calculation domain comprising all the blade. A detailed analysis is given in the impeller inducer and in the vaned diffuser entry region through time-averaged and unsteady flow field. In the impeller inducer, this study demonstrates that the mass flow reduction from peak efficiency to near stall leads to intensification of the secondary flow effects. The low momentum fluid accumulated near the shroud interacts with the main flow through a shear layer zone. At near stall condition, the interface between the two flow structures becomes unstable leading to vortices development. In the diffuser entry region, by reducing the mass flow, the high incidence angle from the impeller exit induces a separation on the diffuser vane suction side. At near stall operating point, vorticity from the separation is shed into vortex cores which are periodically formed and convected downstream along the suction side. 1. Introduction Centrifugal compressors for the aeronautical field are expected to achieve high pressure ratios and high efficiencies at design operating point while minimizing the element size. In this context, typical centrifugal compressor stages are composed of high speed impellers with vaned diffusers to achieve the high pressure recovery in a reduced space. On the other hand, extending the operating range as much as possible is also an important design constraint. As for axial configurations, the limitation at low mass flow rates comes from the rotating stall and/or surge phenomena. Rotating stall is characterized by the presence of one or several cells rotating around the annulus, either in the impeller or in the diffuser. Surge is a system dependant phenomenon associated to large amplitude oscillations of the pressure through the compressor system [1]. The works of Galindo et al. [2] show that the surge intensity can be modified by changing the length of the duct downstream the compressor. However, operating the system in these unstable conditions induces a dramatic drop of performance associated with mechanical stresses that may cause the failure of the compressor. Therefore, a margin (surge margin) is taken to keep away the operating point from these phenomena, leading to an
References
[1]
E. M. Greitzer, “Surge and rotating stall in axial flow compressors, part I: theoretical compression system model,” ASME Journal of Engineering and Power, vol. 98, no. 2, pp. 190–198, 1976.
[2]
J. Galindo, J. R. Serrano, H. Climent, and A. Tiseira, “Experiments and modelling of surge in small centrifugal compressor for automotive engines,” Experimental Thermal and Fluid Science, vol. 32, no. 3, pp. 818–826, 2008.
[3]
N. Cumpsty, Compressor Aerodynamics, Pearson Education, 2004.
[4]
G. J. Skoch, “Experimental investigation of centrifugal compressor stabilization techniques,” Journal of Turbomachinery, vol. 125, no. 4, pp. 704–713, 2003.
[5]
H. W. Emmons, C. E. Pearson, and H. P. Grant, “Compressor surge and stall propagation,” Transaction of the ASME, vol. 77, pp. 455–469, 1955.
[6]
S. Mizuki and Y. Oosawa, “Unsteady flow within centrifugal compressor channels under rotating stall and surge,” Journal of Turbomachinery, vol. 114, no. 2, pp. 312–320, 1992.
[7]
M. P. Wernet, M. M. Bright, and G. J. Skoch, “An investigation of surge in a high-speed centrifugal compressor using digital PIV,” Journal of Turbomachinery, vol. 123, no. 2, pp. 418–428, 2001.
[8]
I. Trébinjac, N. Bulot, X. Ottavy, and N. Buffaz, “Surge inception in a transonic centrifugal compressor stage,” in Proceedings of the ASME Turbo Expo, pp. GT2011–G45116, June 2011.
[9]
T. R. Camp and I. J. Day, “A study of spike and modal stall phenomena in a low-speed axial compressor,” Journal of Turbomachinery, vol. 120, no. 3, pp. 393–401, 1998.
[10]
Z. S. Spakovszky and C. H. Roduner, “Spike and modal stall inception in an advanced turbocharger centrifugal compressor,” Journal of Turbomachinery, vol. 131, no. 3, pp. 1–9, 2009.
[11]
L. Cambier and M. Gazaix, “elsA: an efficient object-oriented solution to CFD complexity,” in Proceedings of the 40th Aerospace Science Meeting and Exhibit, Reno, Nev, USA, 2002.
[12]
P. R. Spalart and S. R. Allmaras, “One-equation turbulence model for aerodynamic flows,” Recherche Aerospatiale, no. 1, pp. 5–21, 1994.
[13]
S. Yoon and A. Jameson, “An LU-SSOR scheme for the Euler and Navier-Stokes equation,” in Proceedings of the AIAA 25th Aerospace Science Meeting, Paper No. 87-0600, Reno, Nev, USA, 2002.
[14]
A. Jameson, “Time dependent calculations using multigrid, with applications to unsteady flows airfoils and wings,” in Proceedings of the 10th AIAA Computational Fluid Dynamics Conference, Paper No. 91-1596, Reno, Nev, USA, 1991.
[15]
F. Sicot, G. Dufour, and N. Gourdain, “A time-domain harmonic balance method for rotor/stator interactions,” Journal of Turbomachinery, vol. 134, no. 1, Article ID 011001, 13 pages, 2012.
[16]
G. Filola, M. C. Le Pape, and M. Montagnac, “Numerical simulations around wing control surfaces,” in Proceedings of the International Conference on Agricultural Statistics (ICAS '04), 2004.
[17]
N. Gourdain, M. Montagnac, F. Wlassow, and M. Gazaix, “High-performance computing to simulate large-scale industrial flows in multistage compressors,” International Journal of High Performance Computing Applications, vol. 24, no. 4, pp. 429–443, 2010.
[18]
G. Dufour, X. Carbonneau, P. Arbez, J. Cazalbou, and P. Chassaing, “Mesh-generation parameters influence on centrifugal compressor simulation for design optimization,” in Proceedings of the ASME Heat Transfer/Fluids Engineering Summer Conference (HT/FED '04), Paper No. 8004-56314, pp. 609–617, July 2004.
[19]
D. Eckardt, “Instantaneous measurements in the jet wake discharge flow of a centrifugal compressor impeller,” ASME Journal of Engineering for Power, vol. 97, pp. 337–346, 1975.
[20]
D. Eckardt, “Detailed flow investigations within a high-speed centrifugal compressor impeller,” Journal of Fluids Engineering, vol. 98, no. 3, pp. 390–402, 1976.
[21]
W. R. Hawthorne, “Secondary vorticity in stratified compressible fluids in rotating systems,” CUED/A-Turbo/TR 63, University of Cambridge, Cambridge, UK, 1974.
[22]
J. M?rz, C. Hah, and W. Neise, “An experimental and numerical investigation into the mechanisms of rotating instability,” Journal of Turbomachinery, vol. 124, no. 3, pp. 367–374, 2002.
[23]
H. Duc Vo, C. S. Tan, and E. M. Greitzer, “Criteria for spike initiated rotating stall,” Journal of Turbomachinery, vol. 130, no. 1, Article ID 011023, 5 pages, 2008.
[24]
R. C. Dean and Y. Senoo, “Rotating wakes in vaneless diffusers,” Journal of Basic Engineering, vol. 82, pp. 573–574, 1960.
[25]
S. Deniz, E. M. Greitzer, and N. A. Cumpsty, “Effects of inlet flow field conditions on the performance of centrifugal compressor diffusers, part 2: straight-channel diffuser,” Journal of Turbomachinery, vol. 122, no. 1, pp. 11–21, 2000.
[26]
J. J. Jinhee Jeong and F. Hussain, “On the identification of a vortex,” Journal of Fluid Mechanics, vol. 285, pp. 69–94, 1995.
[27]
G. Pullan, A. M. Young, I. J. Day, E. M. Greitzer, and Z. S. Spakovszky, “Origins and structure of spike-type rotating stall,” in Proceedings of the ASME Turbo Expo, pp. GT2012–G68707, June 2012.
[28]
J. N. Everitt and Z. S. Spakovszky, “An investigation of stall inception in centrifugal ompressor vaned diffusers,” in Proceedings of the ASME Turbo Expo, pp. GT2011–G46332, June 2011.