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Discussion about the Practice of Using a Heated Surface in Film Cooling Studies

机译:关于在薄膜冷却研究中使用加热表面的实践的讨论

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It is found in many film-cooling experiments and computational analyses that a heated surface is employed to simulate the actual film-cooling condition with a cooling jet and a hot main flow. Considering that the dominant energy passage in turbine airfoil film cooling is always from the hot combustion gas flowing into the airfoil, employing a heated surface to simulate the actual film cooling condition does not provide the correct physics of the heat flow under an actual film cooling condition, and therefore, the results are questionable. The objective of this paper is to investigate the consequent results associated with the practice of employing a heated surface by comparing its result with actual conditions including a conjugate metal wall and internal cooling via a series of computational simulations. When the surface is heated, in some conditions, negative film cooling effectiveness can be found as a result of a higher surface temperature than the main gas stream temperature. This is unrealistic for an operational turbine system. The heated wall acts as an active heat source; as a result, the concept of using the adiabatic wall temperature (T_(aw)) as the driving temperature potential is no longer valid because an artificially created competing heat source is added into the system, and the heat transfer mechanism on the airfoil is not solely determined by T_(aw). Heating the surface to simulate the film cooling boundary condition, although it does not provide correct physics, can provide the heat transfer coefficient value within 10-15% of the value calculated from the correct boundary conditions. Using a heated surface is only correct under one condition: when all the conditions are reversed, i.e. with a hot jet and cold main gas flow. The practice of using a jet flow with the same temperature of the hot gas (isoenergetic jet) to obtain the film heat transfer coefficient will result in about 20-25% discrepancy from the cooling jet case. The uniformly cooled wall cases fair better than heated cases because it provides correct physics in most part of the surface.
机译:在许多薄膜冷却实验和计算分析中发现,采用加热表面来模拟带有冷却射流和热主流的实际薄膜冷却条件。考虑到涡轮机翼型薄膜冷却中的主要能量通道始终来自流入翼型的热燃烧气体,因此采用加热表面模拟实际的薄膜冷却条件不能在实际的薄膜冷却条件下提供正确的热流物理性质。 ,因此结果令人怀疑。本文的目的是通过一系列计算模拟,通过将加热表面的结果与包括共轭金属壁和内部冷却的实际条件进行比较,来研究与使用加热表面的实践相关的结果。当加热表面时,在某些条件下,由于表面温度高于主流温度,因此会发现负膜冷却效果。对于可操作的涡轮系统,这是不现实的。加热的壁用作主动热源。结果,将绝热壁温(T_(aw))用作驱动温度势的概念不再有效,因为系统中添加了人工创建的竞争性热源,而机翼上的传热机制却不再有效完全由T_(aw)确定。加热表面以模拟薄膜冷却边界条件,尽管它不能提供正确的物理条件,但可以提供的传热系数值在根据正确的边界条件计算出的值的10%到15%之内。仅在一种情况下使用加热的表面才是正确的:当所有条件都相反时,即使用热喷射和冷主气流时。使用具有相同温度的热气体的射流(等能量射流)来获得薄膜传热系数的做法将导致与冷却射流情况相差约20-25%。均匀冷却的壁盒比加热的盒要好得多,因为它在表面的大部分区域提供了正确的物理特性。

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