首页> 外文会议>International Conference Boiling Heat Transfer >EXPERIMENTAL STUDY OF NUCLEATE POOL BOILING OF R134a ON A STAINLESS STEEL TUBE (DFG Joint Research Project: Thermo- and Fluiddynamics in Boiling)
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EXPERIMENTAL STUDY OF NUCLEATE POOL BOILING OF R134a ON A STAINLESS STEEL TUBE (DFG Joint Research Project: Thermo- and Fluiddynamics in Boiling)

机译:R134A在不锈钢管中核池沸腾的实验研究(DFG联合研究项目:沸腾中的热和流体动力学)

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Nucleate pool boiling of R134a is studied experimentally in the reduced pressure range 0.03≤p/p_(c)≤0.5 (1.2 bar≤p≤20.3 bar) for heat fluxes from q=100 000 W/m~(2) down to single phase natural convection. Additionally to the heat transfer measurements, nucleation site density, up to (N/A)_(max)≈6000 sites/cm~(2) is measured by an optical method. The test specimen is a horizontal stainless steel tube with an outer diameter d_(o)=15.0mm and a heated length l_(h)=142mm. The heating surface is sandblasted (roughness R_(a)=0.18 μm). The test tube is heated electrically by a cartridge heater with 6.5 mm diameter and a heating power of 1500 W. The wall temperatures are measured by 8 thermocouples, 4 of them arranged 0.9mm below the heated surface and the other 4 arranged 2.8mm below the heated surface. This arrangement allows for the direct measurement of the local radial heat fluxes in four directions (upward, downward, horizontal forward and horizontal backward). The stainless steel pool boiling apparatus ("German standard apparatus") is contained in a precisely temperature-controlled cell with a temperature stability of Δpartial deriv_(air)=0.02 K between the top point of the test installation (the condenser), and its lowest point where the condensed liquid is fed back into the liquid pool. Experimental results: For the highest pressure investigated (p/p_(c)=0.5) and for high heat fluxes (q≥10 000 W/m~(2)), the ratio of the local heat fluxes to the average heat flux is found to be in the range between 0.95 and 1.05, indicating that boiling heat transfer around the test tube is no more influenced by the direction of the gravity field. For lower average heat fluxes, first the local heat flux from the upper side of the tube and then also from the lower side fall below the ratio q_(loc)/q=1; the heat fluxes from the sides rise to higher values. This indicates that two-phase convective heat transfer and/or sliding bubbles effects around the flanks of the tube are dominating. For the lower pressures, the convection dominated region extends to higher heat fluxes. The circumferential variations of the local heat flux observed are mainly attributed to the low thermal conductivity of the wall material. The data for high heat fluxes (where no circumferential variation occurs) are used for in situ evaluation of the thermal conductivity of the stainless steel wall material, resulting in k≈14 W/m K. The thermal conductivity slightly increases with increasing temperature, showing the common behaviour for stainless steel materials in this temperature range. The nucleation site density measurements are performed on the vertical flank of the test tube. The active nucleation sites are found to exhibit a rather strange behaviour on the sandblasted surface. Most of the sites emit only a series of few bubbles and then become inactive for a longer period; seldom a stable nucleation site can be observed.
机译:的R134a的核沸腾通过实验在减压范围0.03≤p/ P_(c)中≤0.5(1.2bar≤p≤20.3巴),用于从Q = 100 000热通量降到单个研究W /米〜(2)相自然对流。此外,对于传热测量,成核位点密度,高达(N / A)_(最大)≈6000点/ cm〜(2)通过光学方法来测定。测试样品是一个水平的不锈钢管,其外径D_(O)=15.0毫米和加热长度L_(H)=142毫米。加热表面进行喷砂(粗糙度= 0.18微米R_())。试管由筒式加热器与6.5mm直径和1500 W的壁温度由热电偶8,测量的加热功率,其中4下方的加热的表面布置0.9毫米和下面的其它4布置2.8毫米电加热加热的表面。这种布置允许局部径向热通量的在四个方向(向上,向下,向前水平和水平向后)的直接测量。不锈钢池沸腾装置(“德国标准装置”)包含在与Δpartialderiv_(空气)的温度稳定性的精确温度控制的小区=测试安装(冷凝器)的顶点之间0.02 K,和其在此收集冷凝的液体被反馈到液体池最低点。实验结果:对于最高压力研究(P / P_(C)= 0.5)和高热通量(q≥10000瓦/米〜(2)),局部热通量的平均热通量的比率为发现在0.95和1.05之间的范围内,这表明没有更多的通过重力场的方向的影响周围的试管即沸腾热传递。对于较低的平均热通量,首先从管的上侧的局部热通量,然后也从下侧落入比Q_下面(LOC)/ Q = 1;从侧面的热通量上升到更高的值。这表明,围绕管的侧面的两相的对流热传递和/或滑动的气泡效应支配。对于较低的压力下,对流为主区域延伸至更高的热通量。磁通观测到的局部的热的圆周变化主要归因于壁材料的低导热性。对于高热通量的数据(在没有圆周变化发生时)在不锈钢壁材料的热导率的原位评价用于,导致k≈14W /米K的热传导率略微随温度的升高而增加,示出了为不锈钢材料在该温度范围内的共同行为。的成核位点密度的测量在测试管的垂直侧面进行。该活化成核位置被发现表现出喷砂表面上的一个相当奇怪的行为。大部分的网站只发射了一系列的几个气泡,然后成为闲置一段较长时间的;很少稳定的成核位点可以观察到。

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