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Conductive sub-layer of twisted-tape-induced swirl-flow heat transfer in vertical circular tubes with various twisted-tape inserts

机译:带有各种扭曲胶带插入物的垂直圆管中扭曲胶带引起的旋流传热的导电子层

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摘要

Abstract Twisted-tape-induced swirl-flow heat transfer due to exponentially increasing heat inputs with various exponential periods ( Q  =  Q ~( 0 ) exp(t/τ) , τ = 6.04 to 23.07 s) and twisted-tape-induced pressure drop was systematically measured for various mass velocities ( G  = 4115 to 13,656 kg/m_(2) s), inlet liquid temperatures ( T ~( in ) = 285.88 to 299.09 K), and inlet pressures ( P ~( in ) = 847.45 to 943.29 kPa) using an experimental water loop flow. Measurements were made over a 59.2-mm effective length and three sections (upper, middle, and lower positions), within which four potential taps were spot-welded onto the outer surface of a 6-mm-inner-diameter, 69.6-mm-heated length, 0.4-mm-thickness platinum circular test tube. Type SUS304 twisted tapes with a width w  = 5.6 mm, a thickness δ ~( T ) = 0.6 mm, a total length l  = 372 mm, and twist ratios y  = 2.39 and 4.45 were employed in this study. The RANS equations (Reynolds Averaged Navier-Stokes Simulation) with a k–ε turbulence model for a circular tube 6 mm in diameter and 636 mm in length were numerically solved for heating of water with a heated section 6 mm in diameter and 70 mm in length using the CFD code, under the same conditions as the experimental ones and considering the temperature dependence of the thermo-physical properties concerned. The theoretical values of surface heat flux q on the circular tubes with twisted tapes with twist ratios y of 2.39 and 4.45 were found to be almost in agreement with the corresponding experimental values of heat flux q , with deviations of less than 30% for the range of temperature difference between the average heater inner surface temperature and the liquid bulk mean temperature ΔT ~( L )[ = T ~( s,av ) - T ~( L ), T ~( L ) = ( T ~( in ) +  T ~( out ))/2] considered in this study. The theoretical values of the local surface temperature T ~( s ), local average liquid temperature T ~( f,av ), and local liquid pressure drop ΔP ~( x )were found to be within almost 15% of the corresponding experimental ones. The thickness of the conductive sub-layer δ ~( CSL )and the nondimensional thickness of the conductive sub-layer y _( + )~( CSL )on the circular tubes with various twisted-tape inserts were determined on the basis of numerical solutions for the swirl velocities u ~( sw )ranging from 5.23 to 21.18 m/s. Correlations between the conductive sub-layer thickness δ ~( CSL )and the nondimensional thickness of the conductive sub-layer y _( + )~( CSL )for twisted-tape-induced swirl-flow heat transfer in a vertical circular tube were derived.
机译:摘要扭曲带引起的旋流传热是由于在不同的指数周期内(Q = Q〜(0)exp(t /τ),τ= 6.04至23.07 s)指数增加的热输入和扭曲带引起的压力系统测量了各种质量流速(G = 4115至13,656 kg / m_(2)s),入口液体温度(T〜(in)= 285.88至299.09K)和入口压力(P〜(in)= 847.45)至943.29 kPa)。在有效长度59.2毫米和三个部分(上部,中间和下部位置)上进行测量,其中四个潜在的分接头点焊到6毫米内径,69.6毫米内径的外表面上。加热长度,厚度为0.4毫米的铂金圆形试管。在本研究中,使用了SUS304扭曲带,其宽度w = 5.6 mm,厚度δ〜(T)= 0.6 mm,总长度l = 372 mm,扭曲比y = 2.39和4.45。数值求解了直径为6毫米,长度为636毫米的圆形管的ak-ε湍流模型的RANS方程(雷诺平均Navier-Stokes模拟),具有ak–ε湍流模型在与实验条件相同的条件下,使用CFD代码,并考虑相关热物理特性的温度依赖性。发现扭曲比y为2.39和4.45的带有扭曲带的圆管表面热通量q的理论值与相应的热通量q实验值几乎一致,在该范围内偏差小于30%平均加热器内表面温度与液体体积平均温度之间的温差ΔT〜(L)[= T〜(s,av)-T〜(L),T〜(L)=(T〜(in)+ T〜(out))/ 2]。发现局部表面温度T〜(s),局部平均液体温度T〜(f,av)和局部液体压降ΔP〜(x)的理论值在相应实验值的几乎15%以内。在数值解的基础上,确定了带有各种扭带插入件的圆管上的导电子层的厚度δ〜(CSL)和导电子层的无量纲厚度y _(+)〜(CSL)旋流速度u〜(sw)在5.23至21.18 m / s之间。推导了在垂直圆管中扭带诱导旋流传热的导电子层厚度δ〜(CSL)与导电子层的无量纲厚度y _(+)〜(CSL)之间的关系。 。

著录项

  • 来源
    《Heat and mass transfer》 |2018年第4期|963-983|共21页
  • 作者

    K. Hata; K. Fukuda; S. Masuzaki;

  • 作者单位

    Graduate School of Marine Sciences, Kobe University;

    Graduate School of Marine Sciences, Kobe University;

    National Institute for Fusion Science;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-18 02:59:50

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