Numerical analysis on cooling performance of quasi-elliptic multi-inclined holes in CMC combustion liner
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摘要:
为了提高陶瓷基复合材料火焰筒壁面的冷却性能,在现有的圆形多斜孔冷却结构的基础上,设计了一种新型类椭圆形多斜孔冷却结构。同时,采用三维数值模拟的方法将两种多斜孔结构的冷却效果进行了对比。结果表明:新型类椭圆斜孔特征模拟件相较于圆孔特征模拟件,壁面高温区域明显变窄,高温热斑减少,温度分布更加均匀;在经纱方向,类椭圆斜孔特征模拟件高应力区域减少,应力集中现象减弱;在纬纱方向,类椭圆斜孔特征模拟件与圆孔特征模拟件均存在高应力区域。
Abstract:In order to improve the cooling performance of ceramic matrix composite combustion liner wall, a new quasi-elliptic multi-inclined hole cooling structure was designed on the basis of the existing circular multi-inclined hole cooling structure. Meanwhile, the cooling effects of two kinds of multi-inclined hole structures were compared by using three-dimensional numerical simulation method. The results showed that: compared with the circular hole feature simulator, the high temperature area on the wall of the new quasi-elliptic inclined hole simulated part was obviously narrower, the hot spots at high temperature were reduced, and the temperature distribution was more uniform. In the warp yarn direction, the high stress area of the simulated part with quasi-elliptic inclined hole features was reduced, and the stress concentration phenomenon was weakened. In the weft yarn direction, the high stress regions in the feature simulators of quasi-elliptic inclined hole and circular hole were found.
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表 1 气膜孔结构参数
Table 1. Structure parameters of film cooling holes
特征模拟件类型 D/mm L/mm α/(°) β/(°) H/P Dp/mm 类椭圆斜孔 0.3 0.6 45 45 0.25 9.5 圆孔 0.6 0 45 0 0.50 9.5 表 2 CMC弹性参数
Table 2. CMC elasticity parameters
参数 数值 参数 数值 ECMC,X/GPa 227.4 μCMC,ZX 0.15 ECMC,Y/GPa 227.4 GCMC,XY/GPa 91.0 ECMC,Z/GPa 50.0 GCMC,YZ/GPa 17.7 μCMC,XY 0.15 GCMC,ZX/GPa 17.7 μCMC,YZ 0.15 注:表中ECMC、μCMC、GCMC分别为CMC的拉伸模量、泊松比和切变模量。 表 3 模型系数
Table 3. Model coefficients
参数 数值 σk 1.0 σε 1.2 C2 1.9 表 4 不同火焰筒特征模拟件表面最大应力
Table 4. Maximum surface stress of different combustion liner-like simulating specimen
MPa 特征模拟件类型 σX,max σY,max τXY,max 圆孔 164 167 88.6 类椭圆斜孔 174 162 118 表 5 SiCf/SiCm材料的强度极限参数
Table 5. Strength limit parameters of SiCf/SiCm
MPa 参数 数值 Xt 220.19 Yt 220.19 S 157.58 -
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