1. National Key Laboratory of Science and Technology on Aero-Engine Aero-thermodynamics, School of Energy and Power Engineering, Beijing University of Aeronautics and Astronautics,Beijing,China,100191
2. Department of Information Network, Dalian Airforce Communicaiton Non-Commissioned Office Academy,Liaoning,Dalian,China,116600
3. Guizhou Aero-Engine Research Institute, Aviation Industry Corporation of China,Guiyang,China,550081
纸质出版:2015
移动端阅览
CAI Xu, LUO Xiang, ZHAO Xi, XU Guo-qiang, CAI Jun. Flow characteristics in a rotor-stator cavity with cooling air inlet at low radius[J]. 航空动力学报, 2015, 30(4): 775-783.
doi: 10.13224/j.cnki.jasp.2015.04.002
CAI Xu, LUO Xiang, ZHAO Xi, XU Guo-qiang, CAI Jun. Flow characteristics in a rotor-stator cavity with cooling air inlet at low radius[J]. 航空动力学报, 2015, 30(4): 775-783. DOI: 10.13224/j.cnki.jasp.2015.04.002.
doi: 10.13224/j.cnki.jasp.2015.04.002 DOI:
Experiments were conducted on a typical rotor-stator system where air entered through an annular slot at low radius and flowed out of the cavity axially through a rim seal between the rotor and the stator. For the seal in this rotor-stator system
the stationary shroud overlapped the rotating one. Pressure distributions at the stator surface and flow resistance coefficients of the rotor-stator cavity with a maximum gap of 67mm were measured under different dimensionless mass flow rates from 1.32×104 to 4.87×104 with a large range of rotational Reynolds numbers from 0.418×106 to 2.484×106. The results show that pressure on the stator surface decreases with the increase of rotational Reynolds number when the dimensionless mass flow rate is below 1.3×104; when the dimensionless mass flow rate is above 3.034×104
the trend reverses. This is the so-called "pressure inversion effect". However
dimensionless pressure does not show the same changes when rotational dynamic pressure is chosen as the denominator. The resistance coefficient of the rotor-stator cavity is determined by the dimensionless mass flow rate and rotational Reynolds number; for practical application
the resistance coefficient can also be estimated by the turbulent flow parameter in the range of turbulent parameter from 0.1 to 1.6.
Experiments were conducted on a typical rotor-stator system where air entered through an annular slot at low radius and flowed out of the cavity axially through a rim seal between the rotor and the stator. For the seal in this rotor-stator system
the stationary shroud overlapped the rotating one. Pressure distributions at the stator surface and flow resistance coefficients of the rotor-stator cavity with a maximum gap of 67mm were measured under different dimensionless mass flow rates from 1.32×104 to 4.87×104 with a large range of rotational Reynolds numbers from 0.418×106 to 2.484×106. The results show that pressure on the stator surface decreases with the increase of rotational Reynolds number when the dimensionless mass flow rate is below 1.3×104; when the dimensionless mass flow rate is above 3.034×104
the trend reverses. This is the so-called "pressure inversion effect". However
dimensionless pressure does not show the same changes when rotational dynamic pressure is chosen as the denominator. The resistance coefficient of the rotor-stator cavity is determined by the dimensionless mass flow rate and rotational Reynolds number; for practical application
the resistance coefficient can also be estimated by the turbulent flow parameter in the range of turbulent parameter from 0.1 to 1.6.
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