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Transport properties of argon at zero density from viscosity-ratio measurements

机译:从粘度比测量中零密度下氩气的传输特性

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We determined the zero-density viscosity eta(Ar)(0,T) and thermal conductivity lambda(Ar)(0,T) of argon with a standard uncertainty of 0.084% in the temperature range 200 K to 400 K. This uncertainty is dominated by the uncertainty of helium's viscosity eta(He)(0,T), which we estimate to be 0.080% based upon the difference between ab initio and experimental values at 298.15 K. Our results may improve (1) the argon-argon interatomic potential, (2) calculated boundary-layer corrections for primary acoustic thermometry, and (3) calibrations of laminar flow meters as well as instruments for measuring transport properties. At 298.15 K, we determined the ratio eta(Ar)(0,298)/eta(He)(0,298) = 1.138 00 +/- 0.000 13 from measurements of the flow rate of these gases through a quartz capillary while simultaneously measuring the pressures at the ends of the capillary. Between 200 K and 400 K, we used a two-capillary viscometer to determine eta(Ar)(0,T)/eta(He)(0,T) = 1.211 67 - 0.820 34 exp(-T/123.78 K) with an uncertainty of 0.024%. From eta(Ar)(0,T)/eta(He)(0,T), we computed eta(Ar)(0,T) using the values of eta(He)(0,T) calculated ab initio. Finally, we computed the thermal conductivity of argon from eta(Ar)(0,T) and values of the Prandtl number that we computed from argon - argon interatomic potentials.
机译:我们确定了200 K至400 K温度范围内的标准不确定度为0.084%的氩气的零密度粘度η(Ar)(0,T)和热导率λ(Ar)(0,T)。由氦粘度eta(He)(0,T)的不确定性所决定,我们根据298.15 K的从头算与实验值之间的差异估计为0.080%。我们的结果可能会改善(1)氩-氩原子间电位,(2)计算出的用于初次声波测温的边界层校正,以及(3)层流流量计以及用于测量传输特性的仪器的校准。在298.15 K处,我们通过测量这些气体通过石英毛细管的流量,同时测量在毛细管的末端。在200 K和400 K之间,我们使用两毛细管粘度计确定eta(Ar)(0,T)/ eta(He)(0,T)= 1.211 67-0.820 34 exp(-T / 123.78 K)不确定度为0.024%。从eta(Ar)(0,T)/ eta(He)(0,T),我们使用从头算出的eta(He)(0,T)的值来计算eta(Ar)(0,T)。最后,我们根据eta(Ar)(0,T)计算出了氩的热导率,并根据氩-氩原子间的电势计算出了普朗特数。

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