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首页> 外文期刊>Periodica Polytechnica. Mechanical Engineering >Commencement and Development Processes of Flow Unsteadiness at Tip Clearance Region of a Low Speed Axial Compressor Rotor Blade Row
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Commencement and Development Processes of Flow Unsteadiness at Tip Clearance Region of a Low Speed Axial Compressor Rotor Blade Row

机译:低速轴向压缩机转子叶片排尖隙区域流动不稳定的开始和开发过程

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摘要

Commencement and development processes of unsteadiness, caused by blade row tip leakage flow in a low speed axial compressor, are investigated and results are presented in this paper. Analyses are based on results obtained through numerical simulation of unsteady three dimensional viscous flows. Discretization of the Navier-Stokes's equations has been carried out based on upwind second-order scheme and k-ω-SST turbulence modeling was used for estimation of eddy viscosity. Three different circumstances, including design point and two near stall conditions are considered for investigation and discussion. Tip leakage flow frequency spectrums were examined through surveying instantaneous static pressure signals imposed on the blades surfaces. Focusing on time dependent flow structure results signified existence of some pressure peaks at near stall conditions. These regions, which are created as a result of interaction between main inflow and tip leakage flow, lead to occurrence of self-induced unsteadiness. However, at design condition, flow is more affected by the main inflow instead of the tip leakage flow. By occurrence of self-induced unsteadiness, which occurs at near stall condition, tip leakage vortex flow starts to fluctuate at a frequency about the blade passing frequency. Further decrease in the flow rate up to a specified value showed no significant variations in the leakage flow frequency, but, on the other hand, magnified amplitudes of this unsteadiness.
机译:由刀片行尖端泄漏流动在低速轴向压缩机中引起的膨胀和开发过程,并在本文中提出了结果。分析基于通过非稳态三维粘性流动的数值模拟获得的结果。基于Upwind二阶方案进行了Navier-Stokes等式的离散化,并且用于估计涡粘度的K-ω-SST湍流建模。三种不同的情况,包括设计点和两个接近的失速条件被认为是调查和讨论。通过测量施加在叶片表面上的瞬时静态压力信号来检查尖端泄漏流频谱。关注时间依赖性流动结构,结果在近代条件下表示存在一些压力峰的存在。这些区域是由于主要流入和尖端泄漏流动之间的相互作用而产生的区域,导致发生自诱导的不稳定性。然而,在设计条件下,流动受到主要流入的影响而不是尖端泄漏流量。通过发生自诱导的不稳定性,在近失速条件下发生,尖端泄漏涡流流动开始在绕刀片通过频率的频率下波动。进一步降低到指定值的流速显示出泄漏流量的显着变化,但另一方面,这种不稳定性的放大幅度。

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