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

机译:气动载荷不均匀对叶片响应的影响

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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:涡轮机叶片始终承受严重的空气动力学负荷。空气动力学载荷是均匀的并且具有谐波性质。谐波特性取决于转子速度和喷嘴数量(叶片数)。这种谐波负载是造成叶片励磁的主要来源。在某些情况下,空气动力学负载不均匀并且沿周向变化。本文讨论了非均匀气动载荷对叶片振动响应的影响。该工作涉及在存在气流的情况下由于进气流畸变而引起的模型叶片强制响应幅度的实验研究。因此,这种受控的进气流变形代表了一种接近实际的环境,其中涉及在气流存在的情况下旋转叶片。制造了一个试验台,包括旋转叶片盘组件,进风口部分(流量可以以递增方式控制或变形),流量调节模块和气动流发生器(带有进气风扇的吸气模块),用于研究在实验室条件下。针对不同的气流速度和叶片转速进行了测试。实验结果表明,当叶片受到不稳定的空气动力载荷时,叶片的响应增加,并且激发了新的频率。响应的大小和与这些新的激发频率相对应的响应随着气流速度的增加而增加。而且,随着流速的增加,新激发频率的数量也增加。

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