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CFD SIMULATION OF JET PULSATION EFFECTS ON FILM COOLING OF FLAT PLATES

机译:襟翼薄膜冷却时射流脉冲效应的CFD模拟

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In this paper fourteen different CFD cases for CFH (cylindrical film hole) and LDIFF (film hole with laterally diffused exit) geometries were conducted to study the film cooling of flat plates. Those cases included different blowing ratios: 0.5, 1.25 and 1.5 and both steady flow and pulsed jets. In the jet pulsation cases the Duty Cycle was taken 50% and the Strouhal number ranged from 0.0119 to 1.0 for the CFH geometry and from 0.0119 to 0.38 for the LDIFF geometry. Fluent commercial code with realizable k - ε turbulence model was used in this study to investigate how the pulsed jet performance was affected by varying: 1) pulsation frequency,2) blowing ratio and 3) jet geometry.For the CFH geometry (B=0.5) the pulsed jet showed lower film cooling effectiveness than the steady state for all cases examined. However, the frequency effects varied according to the downstream location from the jet exit. Immediately near the jet trailing edge the effectiveness increased as the frequency increased. Downstream (x/D above3) the effectiveness for both St=0.0119 and 0.38 almost agreed while lower effectiveness were noted for St= 0.19. For St=1.0, the effectiveness was above the other frequencies (for all x/D values) but still below the steady state ones. As for the LDIFF geometry (B=1.25) the effect of frequency was negligible and the pulsed jet showed lower film cooling effectiveness than the steady state.Two different blowing ratios (0.5 and 1.5) were examined for the CFH geometry. The pulsation had different effects in the two cases. At B=0.5, lower effectiveness performance everywhere was obtained for pulsed cases compared to steady ones. For B=1.5 pulsation results were highly dependent on the frequency. For low frequency (St=0.0119) the effectiveness was below the steady state one for all x/D values. For higher frequency (St=0.38) the effectiveness was higher than thesteady state one for all x/D values. As for St=0.19 and 1.0 the results were in between the above two frequencies.A spatially averaged effectiveness was developed to enable comparing "overall" performance of all cases examined. This was done by choosing an area downstream of the jet that covered from the jet "trailing edge", x/D = 0 to x/D =10 and also covered a 1/2 pitch on both sides of the jet in the spanwise direction. Using the defined spatially averaged effectiveness with 50% of the coolant (Duty Cycle) an overall reduction in the film cooling effectiveness was found to be: 52.73% for the LDIFF (B=1.25), 38.12% for the CFH (B=0.5) and an overall enhancement of 14.77% for the CFH (B=1.5). Knowing that low effectiveness in case of B=1.5, CFH geometry was caused by the jet "lift-off, results above clearly indicate that jet pulsation will be more effective for cases with detached jet under steady state conditions.Although pulsation didn't bring overall benefit to film cooling, there were cases where pulsed jets helped to increase effectiveness over the steady state conditions. Therefore, present results might be useful for evaluation of the effect of pulse frequency on film cooling effectiveness in real life applications, where jets pulse naturally due to the pressure fluctuations in the engine.
机译:本文针对CFH(圆柱形薄膜孔)和LDIFF(具有横向扩散出口的薄膜孔)几何形状进行了14种不同的CFD案例研究了平板的薄膜冷却。这些情况包括不同的吹气比:0.5、1.25和1.5,以及稳定流和脉冲射流。在喷射脉动情况下,占空比为50%,对于CFH几何结构,斯特劳哈尔数的范围为0.0119至1.0,对于LDIFF几何结构,斯特劳哈尔数的范围为0.0119至0.38。本研究中使用了具有可实现的k-ε湍流模型的流利的商业代码,以研究脉冲喷射性能如何受到以下因素的影响:1)脉动频率, 2)吹风比和3)射流几何形状。 对于CFH几何形状(B = 0.5),在所有检查的情况下,脉冲射流均显示出低于稳态的薄膜冷却效率。但是,频率影响会根据射流出口的下游位置而变化。紧随射流后缘,效率随频率增加而增加。下游(上方x / D 3)St = 0.0119和0.38的有效性几乎一致,而St = 0.19的有效性较低。对于St = 1.0,有效性高于其他频率(对于所有x / D值),但仍低于稳态频率。至于LDIFF几何形状(B = 1.25),频率的影响可忽略不计,脉冲射流显示的薄膜冷却效率比稳态低。 对于CFH几何形状,检查了两种不同的吹风比(0.5和1.5)。在这两种情况下,脉动的影响不同。在B = 0.5时,与稳定情况相比,脉冲情况下到处都可获得较低的效能。对于B = 1.5,脉动结果高度依赖于频率。对于低频(St = 0.0119),对于所有x / D值,有效性均低于稳态之一。对于更高的频率(St = 0.38),其有效性高于 所有x / D值均处于稳态1。至于St = 0.19和1.0,结果在上述两个频率之间。 开发了空间平均有效性以比较所有检查案例的“总体”绩效。这是通过选择射流下游的一个区域来完成的,该区域从射流“后缘”覆盖,x / D = 0到x / D = 10,并且在射流方向上还覆盖了射流两侧的1/2节距。使用定义的空间平均效率和50%的冷却剂(占空比),发现薄膜冷却效率的总体下降为:LDIFF(B = 1.25)为52.73%,CFH(B = 0.5)为38.12% CFH总体提高了14.77%(B = 1.5)。知道在B = 1.5的情况下效率低下,CFH几何形状是由射流“升空”引起的,以上结果清楚地表明,射流脉动对于稳态条件下射流分离的情况将更为有效。 尽管脉动并没有为薄膜冷却带来整体利益,但在某些情况下,脉冲射流有助于提高稳态条件下的效率。因此,目前的结果对于评估实际应用中脉冲频率对薄膜冷却效果的影响可能是有用的,在实际应用中,由于发动机压力波动,射流自然产生脉冲。

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