喷嘴叶片叶栅与径向扩散器联合工作模式下的流动特性

A. Lapuzin, V. Subotovich, Y. Yudin, S. Naumenko, Ivan Malymon
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引用次数: 0

摘要

本文给出了某小型燃气轮机与径向扩压器相结合的喷嘴叶栅的研究数据。在4∙105 ~ 106的雷诺数变化范围和0.4 ~ 1.13的减速速度变化范围内,确定了喷嘴叶片叶栅的气动特性。利用积分法和叶栅后的排水条件,推导了各模式下喷嘴叶栅的流量系数。利用可定向气动探头在三种控制模式下获得的流动参数测量数据,计算了动能损失系数和流动角。当叶栅后会聚-发散环形风道膨胀度为1.43时,该风道窄段内的流动被“锁”在叶栅后减速速度为1.127时的模态中。在这样的速度下,雷诺数106对于流量系数是自相似的。当雷诺数较低时,随着雷诺数的减小,所有减小速度值下的流量系数都急剧减小。当雷诺数小于7∙105时,流速增大导致流量系数减小。当这个数字超过8∙105时,速度的增加导致流量系数的增加,直到流动被“困”在喷嘴叶栅中的时刻。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flow Characteristics of the Nozzle Blade Cascade in the Mode of the Joint Operation with the Radial Diffuser
The obtained research data are given for the nozzle cascade used by a small-size gas turbine of an average fanning in combination with the radial diffuser. Aerodynamic characteristics of the nozzle blade cascade were determined in a wide range of a change in the Reynolds number varying from 4∙105 to 106 and the reduced velocity varying in the range of 0.4 to 1.13. The flow rate coefficient of the nozzle cascade was derived for all modes using the integral methods and the drainages behind the cascade. The kinetic energy loss coefficient and the flow angles were calculated using the measurement data of flow parameters in three control modes that were obtained due to the use of orientable pneumometric probes. When the expansion degree of the convergent –divergent annular duct behind the cascade is equal to 1.43 the flow in the narrow section of this duct is “enlocked” in the mode when the reduced velocity behind the cascade is equal to 1.127. At such velocity the Reynolds number 106 is self-similar for the flow rate coefficient. At lower values of Reynolds number, the decrease of it is accompanied by an intensive decrease in the flow rate coefficient for all the values of the reduced velocity. For the Reynolds number lower than 7∙105 an increase in the velocity results in a decreased flow rate coefficient. When this number exceeds 8∙105 an increase in the velocity results in an increase of the flow coefficient up to the moment when the flow is “enlocked” in the nozzle cascade.
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