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Heat transfer distributions around nominal ice accretion shapes formed on a cylinder in the NASA Lewis icing research tunnel

机译:在NASA Lewis结冰研究隧道中的圆柱体上形成的标称积冰形状周围的传热分布

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摘要

Local heat transfer coefficients were obtained on irregular cylindrical shapes which typify the accretion of ice on circular cylinders in cross flow. The ice shapes were grown on a 5.1 cm (2.0 in.) diameter cylinder in the NASA Lewis Icing Research Tunnel. The shapes were 2, 5, and 15 min accumulations of glaze ice and 15 min accumulation of rime ice. Heat transfer coefficients were also measured around the cylinder with no ice accretion. These icing shapes were averaged axially to obtain a nominal shape of constant cross section for the heat transfer tests. Heat transfer coefficients around the perimeter of each shape were measured with electrically heated copper strips embedded in the surface of the model which was cast from polyurethane foam. Each strip contained a thermocouple to measure the local surface temperature. The models were run in a 15.2 x 68.6 cm (6 x 27 in.) wind tunnel at several velocities. Background turbulence in the wind tunnel was less than 0.5 percent. The models were also run with a turbulence producing grid which gave about 3.5 percent turbulence at the model location with the model removed. The effect of roughness was also simulated with sand grains glued to the surface. Results are presented as Nusselt number versus angle from the stagnation line for the smooth and rough models for both high and low levels of free stream turblence. Roughness of the surface in the region prior to flow separation plays a major role in determining the heat transfer distribution.
机译:在不规则的圆柱体形状上获得了局部传热系数,该形状代表了交叉流动时圆柱体上冰的积聚。冰块在NASA Lewis Icing研究隧道的直径为5.1厘米(2.0英寸)的圆柱体上生长。形状分别为2、5和15分钟的釉冰和15分钟的霜冰。还测量了没有结冰的圆柱周围的传热系数。对这些结冰形状进行轴向平均,以得到用于传热测试的恒定横截面的名义形状。用嵌入聚氨酯泡沫铸造的模型表面中的电加热铜带测量每种形状周围的传热系数。每个带包含一个热电偶以测量局部表面温度。这些模型在速度为15.2 x 68.6厘米(6 x 27英寸)的风洞中运行。风洞中的背景湍流小于0.5%。模型还使用产生湍流的网格运行,该网格在移除模型的情况下在模型位置产生了约3.5%的湍流。还用砂粒粘在表面上模拟了粗糙度的影响。对于自由流湍流的高低水平,光滑和粗糙模型的结果以Nusselt数相对于停滞线的角度表示。流动分离之前的区域中的表面粗糙度在确定传热分布中起主要作用。

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