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首页> 外文期刊>International Journal of Heat and Mass Transfer >Effect of inflow swirl on the vane endwall aerothermal performance with endwall misalignment at transonic condition
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Effect of inflow swirl on the vane endwall aerothermal performance with endwall misalignment at transonic condition

机译:跨音速条件下流入涡流对叶片端壁气热性能的影响

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Effect of turbine inlet swirl condition (swirl intensity and orientation) on endwall heat transfer performance with combustor-turbine misalignment at transonic condition was numerically investigated, and coolant injection from combustor-turbine interface was also considered. Simulations with two mainstream swirl numbers (SN) of 0.6 and 1.0, two swirl orientations, two endwall misalignment modes and slot coolant injection were conducted by solving the three-dimensional RANS equations coupled with the Reynolds Stress Turbulence Model (RSM). Computational results indicate that for anticlockwise swirled condition, the averaged Nu number of the high heat transfer attachment region upstream of the leading edge decreases from 4400 to 3100 with the increasing SN from 0.6 to 1.0. Negative incidence is caused at hub followed by a low heat transfer region at pressure side junction. Enhanced horseshoe vortex and mainstream direct attachment enlarge the hot ring (uncooled area around the vane leading edge) when SN = 0.6. As for clockwise swirled condition, positive incidence is caused at hub and can have some effect on reducing the passage crossflow. The pressure side low heat transfer region enlarges under aligned mode but shrinks under misaligned mode compared with anticlockwise condition. Averaged Nu distributes more uniformly along axial direction. The hot ring can only be observed when SN = 0.6 under misaligned condition. For aligned mode, endwall heat transfer at x/C-ax < 1.0 is 30-50% higher for SN = 0.6 than SN = 1.0. When coolant is introduced at the combustor-turbine interface, the heat transfer strength at attachment region is largely reduced. Under aligned condition, coolant tends to eject out between two swirl cores. The majority of the coolant is constrained in the recirculation region by cavity vortices under misaligned mode. Averaged Nu number at the attachment region is 4450 and 3600 under aligned and misaligned mode, respectively. But the averaged Nu number downstream of the passage throat is less than 2000 and distributes uniformly. (C) 2019 Elsevier Ltd. All rights reserved.
机译:数值研究了跨音速条件下涡轮进气道涡流条件(涡流强度和方向)对燃烧室-涡轮未对准的端壁传热性能的影响,并且还考虑了从燃烧室-涡轮界面喷射冷却剂。通过求解三维RANS方程和雷诺应力湍流模型(RSM),进行了两个主流旋流数(SN)为0.6和1.0,两个旋流取向,两个端壁未对准模式和槽冷却液注入的模拟。计算结果表明,在逆时针涡旋条件下,前缘上游高传热连接区域的平均Nu数从4400降低到3100,而SN从0.6升高到1.0。在轮毂处产生负入射,其次是在压力侧连接处的低传热区域。当SN = 0.6时,增强的马蹄涡流和主流直接连接扩大了热环(叶片前缘周围的非冷却区域)。对于顺时针旋转状态,在轮毂处会产生正入射,并可能对减少通道横流产生一定影响。与逆时针状态相比,压力侧低热传递区域在对准模式下增大,但是在未对准模式下减小。平均的Nu沿轴向更均匀地分布。仅当在未对准条件下SN = 0.6时,才能观察到热圈。对于对齐模式,对于SN = 0.6,x / C-ax <1.0的端壁传热要比SN = 1.0高30-50%。当在燃烧器-涡轮界面处引入冷却剂时,附接区域处的传热强度大大降低。在对齐状态下,冷却剂倾向于在两个涡流芯之间喷出。在未对准模式下,大多数冷却剂在腔体涡流的作用下被限制在再循环区域中。在对齐和未对齐模式下,附着区域的平均Nu数分别为4450和3600。但是通道喉下游的平均Nu数小于2000,并且均匀分布。 (C)2019 Elsevier Ltd.保留所有权利。

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