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Heat transfer enhancement in suddenly expanding annular shear-thinning flows

机译:突然扩展的环形剪切稀化流中的传热增强

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Heat transfer enhancement in suddenly expanding annular pipe flows of Newtonian and shear-thinning non-Newtonian fluids is studied within the steady laminar flow regime. Conservation of mass, momentum, and energy equations, along with the power-law constitutive model are numerically solved. The impact of inflow inertia, annular-diameter-ratio, k, power-law index, n, and Prandtl numbers, is reported over the following range of parameters:Re = {50, 100, 150}, k = {0, 0.5, 0.7}; n = {1, 0.8, 0.6}; andPr = {1, 10, 100}. Heat transfer enhancement downstream of the expansion plane, i.e., Nusselt numbers greater than the downstream fully developed value,Nu/Nufd > 1, is only observed forPr = 10 and 100. In general, higher Prandtl numbers, power-law index values, and annular-diameter-ratios, result in more significant heat transfer enhancement downstream of the expansion plane. Heat transfer augmentation, forPr = 10 and 100, increases with the annular-diameter-ratio. For a given annular-diameter-ratio and Reynolds numbers, increasing the Prandtl number fromPr = 10 toPr = 100, always results in higher peakNuvalues,Numax, for both Newtonian and shear-thinning flows. AllNumaxvalues are located downstream of the flow reattachment point, in the case of suddenly expanding round pipe flows, i.e.,κ = 0. However, for suddenly expanding annular pipe flows, i.e., κ = 0.5 and 0.7,Numaxvalues appear upstream the flow reattachment point. ForPr = 10 and 100, shear-thinning flows display two local peakNu/Nufdvalues, in comparison with one peak value in the case of Newtonian flows. The highest heat transfer enhancement,Numax/Nufd ≈ 5, is observed at κ = 0.7, n = 0.6, andPr = 100.
机译:在稳态层流状态下,研究了牛顿流体突然膨胀的环形管道流和剪切稀化的非牛顿流体的传热增强。求解质量,动量和能量方程的守恒,以及幂律本构模型。在以下参数范围内报告了流入惯量,环形直径比,k,幂律指数,n和Prandtl数的影响:Re = {50,100,150},k = {0,0.5 ,0.7}; n = {1,0.8,0.6}; andPr = {1,10,100}。仅在Pr = 10和100时才观察到膨胀平面下游的传热增强,即Nusselt数大于下游的完全展开值Nu / Nufd>1。通常,较高的Prandtl数,幂律指数值和环形直径比,会导致扩展平面下游的传热效果显着提高。对于Pr = 10和100,传热增加随环形直径比而增加。对于给定的环形直径比和雷诺数,将普朗特数从Pr = 10增加到Pr = 100,对于牛顿流和剪切稀化流始终会导致较高的峰值NuuxNumax。在圆管流量突然扩大的情况下,所有Numax值都位于流重新连接点的下游,即κ= 0;而在圆管突然膨胀的情况下,即κ= 0.5和0.7,所有Numax值都出现在流重新连接点的上游。对于Pr = 10和100,剪切稀化流显示两个局部峰值Nu / Nufd值,而在牛顿流中显示一个局部峰值。在κ= 0.7,n = 0.6,Pr = 100时观察到最高的传热增强Numax /Nufd≈≈5。

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