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THE EFFECT OF NON-UNIFORM AERODYNAMIC LOADING ON THE BLADE RESPONSES

机译:非均匀空气动力载荷对叶片响应的影响

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Turbine blades are always subjected to severe aerodynamic loading. The aerodynamic loading is uniform and of harmonic nature. The harmonic nature depends on the rotor speed and number of nozzles (vanes counts). This harmonic loading is the main sources responsible for blade excitation. In some circumstances, the aerodynamic loading is not uniform and varies circumferentially. This paper discussed the effect of the non-uniform aerodynamic loading on the blade vibrational responses. The work involved the experimental study of forced response amplitude of model blades due to inlet flow distortion in the presence of airflow. This controlled inlet flow distortion therefore represents a nearly realistic environment involving rotating blades in the presence of airflow. A test rig was fabricated consisting of a rotating bladed disk assembly, an inlet flow section (where flow could be controlled or distorted in an incremental manner), flow conditioning module and an aerodynamic flow generator (air suction module with an intake fan) for investigations under laboratory conditions. Tests were undertaken for a combination of different air-flow velocities and blade rotational speeds. The experimental results showed that when the blades were subjected to unsteady aerodynamic loading, the responses of the blades increased and new frequencies were excited. The magnitude of the responses and the responses that corresponding to these new excited frequencies increased with the increase in the airflow velocity. Moreover, as the flow velocity increased the number of the newly excited frequency increased.
机译:涡轮叶片始终受到严重的空气动力学载荷。空气动力学载荷是均匀的谐波性质。谐波性质取决于转子速度和喷嘴数量(叶片计数)。这种谐波负载是负责刀片励磁的主要源。在某些情况下,空气动力学负载不均匀并且周向变化。本文讨论了非均匀空气动力载荷对叶片振动反应的影响。工作涉及模型叶片的强制响应幅度的实验研究由于气流存在的入口流动变形。因此,这种受控入口流动变形代表了涉及气流存在下旋转叶片的近乎逼真的环境。由旋转的叶片组件组成的试验台,入口流动部分(可以以增量方式控制或失真),流量调节模块和空气动力流动发生器(带进气风扇的空气吸入模块)进行研究,用于研究在实验室条件下。对不同气流速度和叶片转速的组合进行了测试。实验结果表明,当叶片进行不稳定的空气动力负载时,燃料增加和新频率的响应是兴奋的。随着气流速度的增加,对应于这些新激发频率的响应的幅度和响应增加。而且,随着流速增加的新激励频率的数量增加。

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