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High-speed centrifugal blower for experimental aeroacoustics

High-speed centrifugal blower for experimental aeroacoustics
用于实验气动声学的高速离心鼓风机
批准号:
407546-2011
负责人:
Mohany, Atef
金额:
$1.1万
依托单位:
依托单位国家:
加拿大
项目类别:
Research Tools and Instruments - Category 1 (<$150,000)
财政年份:
2010
资助国家:
加拿大
项目状态:
已结题
起止时间:
2010-01-01 至 2011-12-31

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中文摘要
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英文摘要
The vortex-shedding phenomenon has been a subject of research since it was observed by Leonardo da Vinci. Vortex shedding occurs due to the boundary layer separation around bluff bodies in cross-flow. The boundary layer separates into two shear layers that trail and roll-up in the near field forming a periodic vortex street. In the case of a duct containing a bluff body such as a circular cylinder, when the vortex shedding frequency coincides with one of the acoustic natural frequencies of the duct, a feedback cycle may occur where the vortex shedding acts as a sound source and excites an acoustic standing wave which, in turn, enhances the shedding process and thereby creates a strong acoustic resonance. This process is known as flow-excited acoustic resonance. In many engineering applications where ducts containing clusters of bluff bodies are encountered, such as tube bundles of heat exchangers and boilers, cascades of compressor blades and guide/turning vanes in ducts and radial diffusers, unfortunate operating conditions could lead to a coincidence between the vortex shedding frequency and one of the acoustic natural frequencies of the duct. This often leads to flow-excited acoustic resonance and the generation of acute noise problems and/or excessive vibrations. Since this phenomenon is not yet fully understood, it can be dangerously unpredictable and may cause catastrophic failures in many applications such as power generation and transport. The main objective of the applicant's research in this area is to understand the feedback cycle of the flow-excited acoustic resonance. This requires the generation of a self-excited acoustic resonance in flow configurations similar to those mentioned above. However, the self-excited acoustic resonance will not materialize unless the flow velocity is sufficiently high to overcome the losses due to acoustic damping.This can only be achieved using the requested centrifugal blower system, which is capable of producing air flow with a velocity as high as 220 m/s in a cross-section area of 10 inch (25.4 cm) by 10 inch (25.4 cm).
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Flow-Sound Interaction Mechanisms with Application to Bluff Body Wakes and Separated Shear Flows
Investigation and implementation of pulse-electro thermal de-icing in commercial electric vehicles
Investigation of the Dynamic Characteristics of CANDU Fuel Bundle
Flow-Sound Interaction Mechanisms and Control Strategies
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