期刊文献+
共找到3篇文章
< 1 >
每页显示 20 50 100
不同换算转速对高负荷风扇静子角区流动的影响 被引量:1
1
作者 何成 王如根 +3 位作者 李仁康 宋昊林 何畏 谢祥勇 《推进技术》 EI CAS CSCD 北大核心 2017年第10期2348-2357,共10页
为了探究影响高负荷风扇的失稳机制,对风扇第二级静子叶根角区气流分离的形成原因进行了研究,分析了不同换算转速对角区的流动状态以及壁角涡形成与发展的影响。研究表明,经过静子叶根前缘的气流逐渐发展形成了壁角涡,而壁角涡的存在促... 为了探究影响高负荷风扇的失稳机制,对风扇第二级静子叶根角区气流分离的形成原因进行了研究,分析了不同换算转速对角区的流动状态以及壁角涡形成与发展的影响。研究表明,经过静子叶根前缘的气流逐渐发展形成了壁角涡,而壁角涡的存在促使了静子吸力面角区的气流分离,且随着风扇工况向近失速点移动,更多的角区气流直接参与了壁角涡的形成。在所研究的范围内,换算转速增加会导致壁角涡强度增加、影响范围扩大;在95%~105%换算转速,壁角涡是引起角区气流分离的主要因素,而在85%换算转速,壁角涡已不再是引起角区气流分离和风扇失稳的主要原因。 展开更多
关键词 高负荷风扇 区流动分离 壁角涡 换算转速
原文传递
超高负荷涡轮叶栅内的旋涡结构分析 被引量:3
2
作者 易小兰 张华良 +3 位作者 苏赫 高庆 陈海生 谭春青 《工程热物理学报》 EI CAS CSCD 北大核心 2014年第7期1290-1294,共5页
通过对叶型转折角为160°的超高负荷平面涡轮叶栅内部的流场细节进行数值模拟,将数值模拟结果与流场流线拓扑分析理论相结合,对叶栅内的复杂旋涡结构进行定性分析,详述超高负荷平面涡轮叶栅内马蹄涡、通道涡、壁角涡、尾缘涡和端壁... 通过对叶型转折角为160°的超高负荷平面涡轮叶栅内部的流场细节进行数值模拟,将数值模拟结果与流场流线拓扑分析理论相结合,对叶栅内的复杂旋涡结构进行定性分析,详述超高负荷平面涡轮叶栅内马蹄涡、通道涡、壁角涡、尾缘涡和端壁二次涡等涡系的产生、发展和演化过程,以及它们之间的相互作用关系;在此基础上,通过总压损失系数分布和出口截面涡量分布给出定量分析。 展开更多
关键词 超高负荷 分离 通道 壁角涡
原文传递
Turbine Endwall Film Cooling With Combustor-Turbine Interface Gap Leak- age Flow: Effect of Incidence Angle 被引量:1
3
作者 ZHANG Yang YUAN Xin 《Journal of Thermal Science》 SCIE EI CAS CSCD 2013年第2期135-144,共10页
This paper is focused on the film cooling performance of combustor-turbine leakage flow at off-design condition. The influence of incidence angle on film cooling effectiveness on first-stage vane endwall with combusto... This paper is focused on the film cooling performance of combustor-turbine leakage flow at off-design condition. The influence of incidence angle on film cooling effectiveness on first-stage vane endwall with combustor-turbine interface slot is studied. A baseline slot configuration is tested in a low speed four-blade cascade comprising a large-scale model of the GE-E 3 Nozzle Guide Vane (NGV). The slot has a forward expansion angle of 30 deg. to the endwall surface. The Reynolds number based on the axial chord and inlet velocity of the free-stream flow is 3.5 × 10 5 and the testing is done in a four-blade cascade with low Mach number condition (0.1 at the inlet). The blowing ratio of the coolant through the interface gap varies from M = 0.1 to M = 0.3, while the blowing ratio varies from M = 0.7 to M = 1.3 for the endwall film cooling holes. The film-cooling effectiveness distributions are obtained using the pressure sensitive paint (PSP) technique. The results show that with an increasing blowing ratio the film-cooling effectiveness increases on the endwall. As the incidence angle varies from i = +10 deg. to i = 10 deg., at low blowing ratio, the averaged film-cooling effectiveness changes slightly near the leading edge suction side area. The case of i = +10 deg. has better film-cooling performance at the downstream part of this region where the axial chord is between 0.15 and 0.25. However, the disadvantage of positive incidence appears when the blowing ratio increases, especially at the upstream part of near suction side region where the axial chord is between 0 and 0.15. On the main passage endwall surface, as the incidence angle changes from i = +10 deg. to i = 10 deg., the averaged film-cooling effectiveness changes slightly and the negative incidence appears to be more effective for the downstream part film cooling of the endwall surface where the axial chord is between 0.6 and 0.8. 展开更多
关键词 Film Cooling ENDWALL Pressure Sensitive Paint Leakage Flow
原文传递
上一页 1 下一页 到第
使用帮助 返回顶部