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      Numerical Simulation of the Thermal Conductivity of Thermal Insulation Pipe by Vacuum and High Pressure Argon Pre—filled

      2014-10-21 12:49:13ZHOUCheng-longXUYong-xiangSHENGHong-zhi
      科技視界 2014年34期
      關(guān)鍵詞:責(zé)任

      ZHOU Cheng-long XU Yong-xiang SHENG Hong-zhi

      【Abstract】By analyzing the insulation effect of argon-filled tubing and vacuum-insulated tubing before and after hydrogen permeation respectively, a conclusion can be drawn that the insulated tubing filled with high pressure argon is better than the vacuum insulated tubing considering the lifetime and heat insulation effect.

      【Key words】Hydrogen permeation;Vacuum insulated tubing;Argon filled tubing;Thermal conductivity

      1 Comparison of the hydrogen permeation rate of the argon filled tubing and the vacuum insulated tubing

      Figure.1 The principle diagram of the hydrogen permeation

      From the microscopic point of view, hydrogen permeation process is carried out according to the following steps[1-3]:

      First, the hydrogen molecules impact to the outer surface of the vacuum environment, and adsorbed by the outer surface;

      Second, part of the hydrogen molecules which are absorbed by the outer surface can be dissociated into atomic state;

      Third, hydrogen atoms reaches an equilibrium solubility on the outer surface;

      Fourth, because of the existence of concentration gradient, hydrogen atoms are diffused to the surface of the vacuum side;

      Fifth, hydrogen atoms are released into the vacuum environment after combined into the molecular state.

      According to the law of diffusion, the formula of permeation rate of gas can be deduced:

      Q=■(8)

      Q——permeation rate of gas;

      K——permeability coefficient of a gas to a solid;

      A——area of surface;

      Δp——the difference of gas pressure between two sides of the wall;

      j——dissolution constant, if the solid is metal and the gas is diatomic molecule, such as hydrogen, j=2;

      h——wall thickness.

      According to the above formula, we can see that the rate of hydrogen permeation(Q) is proportional to the pressure difference of 1/2 times (Δp)1/2. Existing in the insulated tubing is about 350℃ water vapor, and its pressure is about 21MPa. The pressure of argon filled tubing is about 1MPa, and the pressure of vacuum insulated tubing is close to 0. Therefore, we may safely draw the conclusion that ?p of the argon filled tubing is smaller than that of the vacuum insulated tubing, so, permeation rate(Q) of the argon filled tubing is smaller than that of the vacuum insulated tubing, namely hydrogen permeation of the argon filled tubing is slower than that of the vacuum insulated tubing.

      2 Thermal conductivity of N80 steel, H2, Ar and H2-Ar gas mixture at different temperatures

      According to the chemical compositions, standard steels can be classified into three major groups: carbon steels, alloy steels, and stainless steels. Carbon Steels are defined as follows[4]: alloying elements do not exceed these limits: 1% carbon, 0.6%copper, 1.65% manganese, 0.4% phosphorus, 0.6%silicon, and0.05%sulfur.

      According to the N80 steels from Sumitomo, Mannesmann, the United States, the Czech Republic and other places, we can get its chemical compositions:0.3%-0.4% carbon, 0.02% copper, 1.25%-1.62% manganese, 0.013%-0.022% phosphorus, 0.25%-0.38% silicon, 0.005%-0.008% sulfur, therefore, it can be concluded that N80 is a typical carbon steel.

      Carbon content is the main factors affecting the thermal conductivity of carbon steel[5]. Smithells Metals Reference Book[6] has provided the thermal conductivity of carbon steel whose carbon content is 0.4%, its value is as follows:

      Table 1

      Table 1 thermal conductivity of N80 steel as the change of temperature

      The thermal conductivity of H2, Ar and H2-Ar gas mixture at different temperatures has been calculated in another paper[7].

      3 The results and analysis of numerical simulation

      The following two figure are the temperature maps and the heat-flux maps of the vacuum insulated tubing of C level-whose thermal conductivity(λ) is 0.02:

      Figure.2 Temperature maps

      Figure.3 heat-flux maps

      Besides, heat-flux densities of vacuum insulated tubing at different levels were calculated, as shown in the following table:

      Table 2

      Table 2 heat-flux densities of vacuum insulated tubing at different levels

      In addition, the heat-flux density of argon filled tubing containing different content of hydrogen were calculated, as shown in the following table:

      Table 3

      Table 3 Heat-flux of argon filled tubing containing different content of hydrogen

      By comparing the tables of (2) and (3), we can see that the insulation effect of argon filled tubing is slightly inferior to the vacuum insulated tubing of C class at the initial stage, however, it is enough to meet the requirement of thermal insulation effect.

      When a certain amount of hydrogen is penetrated, the heat-flux density of the vacuum insulated tubing will reach to more than 13 thousand, so, the tubing cannot meet the requirements of thermal insulation effect at all.

      However, when the content of hydrogen permeated into the argon filled tubing is above 40%, the tubing will be near to the critical value of failure. So that the heat insulated tubing life is greatly extended in the premise of perfect heat insulation effect. Therefore, the insulated tubing filled with high pressure argon is better than the vacuum insulated tubing considering the lifetime and heat insulation effect.

      【Reference】

      [1]Kurt S. Rothenberger, Bret H. Howard, Richard P. Killmeyer, Anthony V. Cugini, Robert M. Enick, Felipe Bustamante, Michael V. Ciocco, Bryan D. Morreale, Robert E. Buxbaum, Evaluation of tantalum-based materials for hydrogen separation at elevated temperatures and pressures[J].Journal of Membrane Science, 2003,218(1-2):19-37.

      [2]Bryan D. Morreale, Michael V. Ciocco, Robert M. Enick, Badi I. Morsi, Bret H. Howard, Anthony V. Cugini, Kurt S. Rothenberger, The permeability of hydrogen in bulk palladium at elevated temperatures and pressures[J].Journal of Membrane Science, 2003,212(1-2):87-97.

      [3]Timothy L. Ward, Tien Dao, Model of hydrogen permeation behavior in palladium membranes[J].Journal of Membrane Science,1999,153(2):211-231.

      [4]Efundawebsite,2009.[OL].

      [5]Meng Yuyong,Wang Jianjun,Zhou Li,Wang Xianghong. Study on Relationship between Temperature and Thermal Conductivity in Different Kinds of Steel[J].Iron Steel Vanadium Titanium, 2013, 34(3):97-100.

      [6]T. C. Totmeier, W. F. Gale, Smithells Metals Reference Book[M].Butterworth - Heinemann,2004.

      [7]Chenglong Zhou, Yongxiang Xu, Hongzhi Sheng. Calculation of thermal conductivity of hydrogen-argon gas mixture at different temperatures[J].Science & Technology Vision,2014,11.

      [責(zé)任編輯:薛俊歌]

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