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首页> 外文期刊>Bulletin of the American Physical Society >APS -70th Annual Meeting of the APS Division of Fluid Dynamics- Event - Bending mode flutter in a transonic linear cascade
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APS -70th Annual Meeting of the APS Division of Fluid Dynamics- Event - Bending mode flutter in a transonic linear cascade

机译:APS -70TH APS划分的APS划分的年会 - 事件 - 弯曲模式在横向线性级联中扑振

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摘要

Vibration related issues like flutter pose a serious challenge to aircraft engine designers. The phenomenon has gained relevance for modern engines that employ thin and long fan blade rows to satisfy the growing need for compact and powerful engines. The tip regions of such blade rows operate with transonic relative flow velocities, and are susceptible to bending mode flutter. In such cases, the flow field around individual blades of the cascade is dominated by shock motions generated by the blade motions. In the present work, a new transonic linear cascade facility with the ability to oscillate a blade at realistic reduced frequencies has been developed. The facility operates at a Mach number of 1.3, with the central blade being oscillated in heave corresponding to the bending mode of the rotor. The susceptibility of the blade to undergo flutter at different reduced frequencies is quantified by the cycle-averaged power transfer to the blade calculated using the measured unsteady load on the oscillating blade. These measurements show fluid excitation (flutter) at low reduced frequencies and fluid damping (no flutter) at higher reduced frequencies. Simultaneous measurements of the unsteady shock motions are done with high speed shadowgraphy to elucidate the differences in shock motions between the excitation and damping cases.
机译:振动相关问题,如扑腾为飞机发动机设计师构成了严峻挑战。该现象对现代发动机的相关性,采用薄而长的风扇刀片行,以满足压缩和强大的发动机的日益增长的需求。这种刀片行的尖端区域用横向相对流速操作,并且易于弯曲模式颤动。在这种情况下,级联的各个叶片周围的流场由由刀片运动产生的冲击运动为主。在本作工作中,已经开发出一种新的跨音质线性级联设施,其具有在现实降低的频率下振荡刀片的能力。该设施在马赫数为1.3的马赫数,中央刀片在对应于转子的弯曲模式的升降中振荡。通过使用在振荡刀片上测量的不稳定负载计算的循环平均功率传输来量化叶片以发生不同减小的频率的颤动的磁颤。这些测量显示在低减小的频率下的流体激发(颤动)和更高的频率下的流体阻尼(无颤动)。不稳定的震动运动的同时测量是用高速影子图进行的,以阐明激发和阻尼盒之间的冲击运动的差异。

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