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SCALING HEAT-TRANSFER COEFFICIENTS MEASURED UNDER LABORATORY CONDITIONS TO ENGINE CONDITIONS

机译:在实验室条件下对发动机条件测得的比例传热系数

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Almost all measurements of the heat-transfer coefficient (HTC) or Nusselt number (Nu) in gas-turbine cooling passages with heat-transfer enhancement features such as pin fins and ribs have been made under conditions, where the wall-to-bulk temperature, T_w/T_b, is near unity. Since T_w/T_b in gas-turbine cooling passages can be as high as 2.2 and vary appreciably along the passage, this study examines if it is necessary to match the rate of change in T_w/T_b when measuring Nu, whether Nu measured at T_w/T_b near unity needs to be scaled before used in design and analysis of turbine cooling, and could that scaling for ducts with heat-transfer enhancement features be obtained from scaling factors for smooth ducts because those scaling factors exist in the literature. In this study, a review of the data in the literature shows that it is unnecessary to match the rate of change in T_w/T_b for smooth ducts at least for the rates that occur in gas turbines. For ducts with heat-transfer enhancement features, it is still an open question. This study also shows Nu measured at T_w/T_b near unity needs to be scale to the correct T_w/T_b before it can be used for engine conditions. By using steady RANS analysis of the flow and heat transfer in a cooling channel with a staggered array of pin fins, the usefulness of the scaling factor, (T_w/T_b)~r, from the literature for smooth ducts was examined. Nu_(engine), computed under engine conditions, was compared with those computed under laboratory conditions, Nu_(lab), and scaled by (T_w/T_b)~r; i.e., Nu_(lab,scaled) = Nu_(lab) (T_w/T_b)~r. Results obtained show the error in Nu_(lab,scaled) relative to Nu_(engine) can be as high as 36.6% if r = -0.7 and T_w/T_b = 1.573 in the "fully" developed region. Thus, (T_w/T_b)~r based on smooth duct should not be used as a scaling factor for Nu in cooling passages with heat-transfer enhancement features. To address this inadequacy, a method is proposed for generating scaling factors, and a scaling factor was developed to scale the heat transfer from laboratory to engine conditions for a channel with pin fins.
机译:在具有壁传热温度的条件下,几乎所有具有传热增强功能的燃气轮机冷却通道中的传热系数(HTC)或努塞尔数(Nu)都已测量,例如针状翅片和肋条。 T_w / T_b接近于1。由于燃气轮机冷却通道中的T_w / T_b可能高达2.2,并且沿通道有明显变化,因此本研究研究了在测量Nu时是否必须匹配T_w / T_b的变化率,Nu是否以T_w /在用于涡轮机冷却的设计和分析之前,需要对接近于T的b进行缩放,并且可以从光滑导管的缩放因子中获得具有传热增强功能的导管的缩放比例,因为这些缩放因子存在于文献中。在这项研究中,对文献中数据的回顾表明,至少对于燃气轮机中发生的速率,无需匹配光滑管道的T_w / T_b变化率。对于具有传热增强功能的风管,这仍然是一个悬而未决的问题。这项研究还表明,在T_w / T_b接近于1的情况下测得的Nu必须先缩放到正确的T_w / T_b,然后才能用于发动机工况。通过对带有交错排列的针状翅片的冷却通道中的流动和传热进行稳定的RANS分析,检验了文献中用于平滑风道的比例因子(T_w / T_b)〜r的有用性。将在发动机条件下计算的Nu_(engine)与在实验室条件下计算的Nu_(lab)进行比较,并按(T_w / T_b)〜r进行缩放;即Nu_(lab,scaled)= Nu_(lab)(T_w / T_b)〜r。获得的结果表明,如果在“完全”发达的地区,如果r = -0.7且T_w / T_b = 1.573,则Nu_(lab,scaled)相对于Nu_(engine)的误差可能高达36.6%。因此,不应将基于光滑管道的(T_w / T_b)〜r用作具有传热增强功能的冷却通道中Nu的比例因子。为了解决这一不足,提出了一种生成缩放因子的方法,并且开发了缩放因子来缩放具有针状翅片的通道从实验室到发动机工况的热传递。

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