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Measurement of heat transfer coefficient in two phase flows of radiation-resistant zeotropic C_2F_6/C_3F_8 blends

机译:抗辐射共沸C_2F_6 / C_3F_8共混物两相流传热系数的测量

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摘要

We have measured the flow boiling heat transfer coefficient (HTC) of saturated fluorocarbon blends in a horizontal copper-nickel tube with a diameter of 4 mm. Direct (Joule) heating of the tube wall was used to obtain heat fluxes from 5 to 13.7 kWm~(-2). Two different injection capillaries were used, permitting measurements at mass fluxes varying between 94 and 164 kg m~(-2)s~(-1). The evaporation pressure was approximately 0.2 MPa for the mass fluxes close to 164 kg m~(-2) s~(-1) and 0.15 MPa for the lower mass fluxes. The same tube dimensions and material are used in the on-detector cooling channels of the silicon micro-strip charged particle tracker ("SCT") of the ATLAS experiment at the CERN Large Hadron Collider. The range of heat flux and mass flow studied encompasses the operating conditions of the tracker. When operating in the high radiation environment near to the proton beam collisions radiation tolerant coolants are essential. Saturated fluorocarbons (C_nF_((2n+2))) are radiation resistant and allow thermodynamic "tailoring" by blending saturated molecules of different orders. Measurements were made with pure C_3F_8 (R218) and zeotropic blends containing 5,10,15,20 and 25% (molar) C_2F_6 (R116). This work is a continuation of a previous study which showed that the operating temperature of the ATLAS SCT could be reduced by around 10 ℃ with the admixture of 25% (molar) C_2F_6, with no changes needed to the existing on-detector and circulatory pipework. The data analysis revealed multiple flow boiling regimes of the two-phase flow that varied as a function of coolant flow rate, heat flux, vapour quality and mixture composition. As expected, the HTC in pure C_3F_8 was higher than in blends with increasing C_2F_6 content. Nevertheless, the study confirmed that the ATLAS SCT could be operated at full power dissipation with cooling tube temperatures up to 10 ℃ colder than in pure C_3F_8 with C_3F_8/C_2F_6 blends having relatively modest values of HTCs in the range 1500-4000 W m~(-2) K~(-1).
机译:我们已经在直径为4 mm的水平铜镍管中测量了饱和碳氟化合物混合物的沸腾沸腾传热系数(HTC)。管壁的直接(焦耳)加热用于获得5至13.7 kWm〜(-2)的热通量。使用了两种不同的注入毛细管,可以在94至164 kg m〜(-2)s〜(-1)之间的质量通量下进行测量。对于接近164 kg m〜(-2)s〜(-1)的质量通量,蒸发压力约为0.2 MPa,对于较低的质量通量,蒸发压力约为0.15 MPa。在CERN大型强子对撞机的ATLAS实验的硅微带电粒子跟踪器(“ SCT”)的探测器上冷却通道中使用了相同的管尺寸和材料。研究的热通量和质量流量范围涵盖了跟踪器的工作条件。在接近质子束碰撞的高辐射环境中运行时,耐辐射的冷却剂至关重要。饱和碳氟化合物(C_nF _((2n + 2)))耐辐射,并且可以通过混合不同顺序的饱和分子进行热力学“定制”。使用纯C_3F_8(R218)和含5、10、15、20和25%(摩尔)C_2F_6(R116)的共沸混合物进行测量。这项工作是先前研究的延续,该研究表明,在掺入25%(摩尔)的C_2F_6的情况下,ATLAS SCT的工作温度可以降低10℃左右,而无需改变现有的探测器和循环管道。数据分析表明,两相流的多种沸腾形式随冷却剂流速,热通量,蒸气质量和混合物组成的变化而变化。不出所料,纯C_3F_8中的HTC高于C_2F_6含量增加的共混物中的HTC。尽管如此,该研究证实,ATLAS SCT可以在全功率下运行,其冷却管温度比纯C_3F_8和C_3F_8 / C_2F_6混合物中HTC值相对适中的纯C_3F_8处于1500-4000 W m〜( -2)K〜(-1)。

著录项

  • 来源
    《International Journal of Heat and Mass Transfer》 |2017年第10期|246-256|共11页
  • 作者单位

    Czech Technical University in Prague, Department of Applied Physics, Technicka 4, 166 07 Prague 6, Czech Republic;

    Czech Technical University in Prague, Department of Applied Physics, Technicka 4, 166 07 Prague 6, Czech Republic;

    Czech Technical University in Prague, Department of Applied Physics, Technicka 4, 166 07 Prague 6, Czech Republic;

    CERN, 1211 Geneva 23, Switzerland;

    Aix Marseille Universite, CNRS/IN2P3, CPPM UMR 7346, 13288 Marseille, France;

    B.P. Konstantinov Petersburg Nuclear Physics Institute (PNPI), 188300 St. Petersburg, Russia;

    Department of Physics and Astronomy, Cavendish Laboratory, J.J. Thompson Avenue, University of Cambridge, Cambridge CB3 0HE, UK;

  • 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

    Zeotropic blends; Octafluoropropane; Hexafluoroethane; Boiling HTC; ATLAS SCT; Silicon detector cooling;

    机译:共沸混合物;八氟丙烷;六氟乙烷;沸腾的HTC;ATLAS SCT;硅探测器冷却;

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