Abstract

To investigate unsteady interaction mechanism between the rim seal flow in turbine stator-rotor cavity and main flow, detailed unsteady numerical simulations of the flow field and unsteady characteristic of the vane were conducted under different rim seal mass flow rate. The results show the blockage effect resulting from the egress flow leads to the pressure to increase and static entropy to reduce on the latter half of suction side near the hub. From the case without a cavity to RI=1.7%, at 5% span, the maximum pressure coefficient increase on the suction side reaches 6%. Moreover, the blockage effect causes the velocity to decrease at vane exit. Furthermore, the rim seal flow results in the decrease in lateral pressure gradient, causing the strength of hub passage vortex and hub trailing shedding vortex to reduce. Without rim seal flow, the ingress flow contributes to decreasing unsteady fluctuation from the hub to 10% span. When there is rim seal flow, unsteady fluctuation continues to reduce due to coupling effects of the egress flow from the ingress and the egress flow form the cavity inlet.

Highlights

  • 西北工业大学学报 Journal of Northwestern Polytechnical University https: / / doi.org / 10.1051 / jnwpu / 20193710129

  • To investigate unsteady interaction mechanism between the rim seal flow in turbine stator⁃rotor cavity and main flow, detailed unsteady numerical simulations of the flow field and unsteady characteristic of the vane were conducted under different rim seal mass flow rate

  • The results show the blockage effect resulting from the egress flow leads to the pressure to increase and static entropy to reduce on the latter half of suction side near the hub

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Summary

Introduction

西北工业大学学报 Journal of Northwestern Polytechnical University https: / / doi.org / 10.1051 / jnwpu / 20193710129 流明显增强,如 0 / 5Tr 时刻所示。 总的来说,燃气入 侵基本发生在导叶尾迹区域,封严出流基本发生在 图 10 给出了 6 种工况下导向器出口轴向涡量 的云图。 可以发现,轮毂到 10%叶高之间存在明显 的负涡量结构,是由马蹄涡压力面分支和吸力面分 支汇合形成,称为轮毂通道涡 ( hub passage vortex, HPV) 。 10%叶高到 20% 叶高之间存在明显的正涡 量结构,是由轮毂通道涡和吸力面边界层交互作用 并在导叶尾缘脱落形成,称为轮毂尾缘脱落涡( hub trailing shedding vortex,HTSV) 。 随着封严流量的增 为了更加直观和定量地观察非定常波动的水 平,图 13 给出了 3 种工况下导向器出口 5% 叶高位 置的时均和时刻的静压系数分布,5% 叶高位置如图 13a) 所示。 静压系数由当地静压通过主流进口总 压无量纲化获得。 可以发现,无封严腔体时,由于转 静干涉作用,导叶尾迹区域和通道中间都出现了静 压波动, 相应的波动水平量化后分别为 0.

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