Presently design of anti-icing systems for aircraft engines is generally made for small droplet icing conditions. However, recent research shows that icing accretion due to supercooled large droplet (SLD) may result in extremely severe aircraft or engine performance degradation. With reference to the impact behavior of SLD on an aero-engine strut surface, a numerical method is presented in this paper to model some important phenomena and effects for the SLD, including deforming, breakup, splashing, rebounding, etc. Some semi-empirical computational models drawn from the literature are incorporated into the Eulerian droplet field equations. Comparisons are then made between the impingement characteristics on struts surface in two different regulated angles with an icing cloud median volumetric dimeter (MVD) of 120 μm. Results show that, when the regulated angle is 0°, some smaller droplets are formed because of the breakup effect. Also, due to the splashing and rebounding influence the droplet collection efficiency and impingement limit decrease by 11.8% and 35.7%, respectively. In contrast, no breakup phenomenon is observed when the regulated angle is 30°, and all the impacting mass rebounds away from the regulated surface.
HU Jianping, LIU Zhenxia, ZHANGL Lifen
. Supercooled Large Droplet Impact Behaviors on an Aero-engine Strut[J]. ACTA AERONAUTICAET ASTRONAUTICA SINICA, 2011
, 32(10)
: 1778
-1785
.
DOI: CNKI:11-1929/V.20110426.1307.004
[1] Broeren A P, LaMarre C M, Bragg M B, et al. Characteristics of SLD ice accretions on airfoils and their aerodynamic effects. AIAA-2005-75, 2005.
[2] Anderson D N, Tsao J C. Additional results of ice-accretion scaling at SLD conditions. AIAA-2003-390, 2003.
[3] Marwitz J, Politovich M, Berstein B, et al. Meteorological conditions associated with the ATR72 aircraft accident near roselawn[J]. Bulletin of the American Meteorological Society, 1997, 78(1): 41-52.
[4] Hill E G. Overview of federal aviation administration aviation safety research for aircraft icing. AIAA-2006-81, 2006.
[5] Thomas H B, Dean R M, Mark G P. Overview of SLD engineering tools development. AIAA-2003-386, 2003.
[6] William B W, Mark G P. Semi-empirical modeling of SLD physics. AIAA-2004-412, 2004.
[7] Raimund H, Wagdi G H. Fensap-ice: Eulerian modeling of droplet impingment in the SLD regime of aircraft icing. AIAA-2006-465, 2006.
[8] Iuliano E, Mingione G, Petrosino F. Eulerian modeling of SLD physics towards more realistic aircraft icing simulation. AIAA-2010-7676, 2010.
[9] ANSYS Inc. ANSYS fluent 12.0 user's guide[M]. New Hapmpshire: ANSYS Inc, 2009.
[10] Clift R, Grace J R, Weber M E. Further refinement of the LEWICE SLD model. AIAA-2006-464, 2006.
[11] Hsiang L P, Faeth G M. Second drop breakup in the deformation regime. AIAA-1992-110, 1992.
[12] Tan S C, Papadakis M, Miller D. et al. Experimental study of large droplet splashing and breakup. AIAA-2007-904, 2007.
[13] Geoffrey L, David W H, Paul I. Modeling imaging and measurement of distortion drag and break-up of aircraft-icing droplets. AIAA-2005-71, 2005.
[14] Trujillo M F, Mathews W S, Lee C F, et al. Modeling and experiment of impingment and atomization of a liquid spray on a wall[J]. International Journal of Engine Research, 2000, 1(1): 87-105.
[15] Mundo C, Tropea C, Sommerfeld M. Numerical and experimental investigation of spray characteristics in the vicinity of a rigid wall[J]. Experimental Thermal and Fluid Science, 1997, 15(3): 228-237.
[16] Bai C, Gosman A D. Development of methodology for spray impingement simulation. SAE Technical Paper 950283, 1995.
[17] Cossali G E, Coghe A, Marengo M. The impact of a single drop on a wetted solid surface, experiments on a NACA23012 airfoil with simulated glaze ice shapes. AIAA-2004-506, 2004.
[18] Kuohsing E H, Giao T V, Colin S B. Water droplet impingement on simulated glaze, mixed, and rime ice accre-tions. NASA TM-2007-213961, 2007.