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Determination of the Boltzmann constant with cylindrical acoustic gas thermometry: new and previous results combined

机译:用圆柱声气体测温测定螺栓恒曼常数:新的和以前的结果

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摘要

We report a new determination of the Boltzmann constant k(B) using a cylindrical acoustic gas thermometer. We determined the length of the copper cavity from measurements of its microwave resonance frequencies. This contrasts with our previous work (Zhang et al 2011 Int. J. Thermophys. 32 1297, Lin et al 2013 Metrologia 50 417, Feng et al 2015 Metrologia 52 S343) that determined the length of a different cavity using two-color optical interferometry. In this new study, the half-widths of the acoustic resonances are closer to their theoretical values than in our previous work. Despite significant changes in resonator design and the way in which the cylinder length is determined, the value of k(B) is substantially unchanged. We combined this result with our four previous results to calculate a global weighted mean of our k(B) determinations. The calculation follows CODATA's method (Mohr and Taylor 2000 Rev. Mod. Phys. 72 351) for obtaining the weighted mean value of k(B) that accounts for the correlations among the measured quantities in this work and in our four previous determinations of k(B). The weighted mean (k(B)) over cap is 1.3806484(28) x 10(-23) J K-1 with the relative standard uncertainty of 2.0 x 10(-6). The corresponding value of the universal gas constant is 8.314459(17) J K- 1 mol(-1) with the relative standard uncertainty of 2.0 x 10(-6).
机译:我们通过圆柱声气体温度计报告了Boltzmann常数K(b)的新测定。我们确定了铜腔的长度从其微波谐振频率的测量值。这与我们之前的工作形成鲜明对比(Zhang等,J. Thermophys。32 1297,Lin等人2013 Metrologia 50 417,Feng等人2015 Metrologia 52 S343)使用双色光学干涉测定不同腔的长度。在这项新研究中,声谐振的半宽度更接近其理论值,而不是我们以前的工作。尽管谐振器设计的显着变化和确定汽缸长度的方式,但K(B)的值基本上不变。我们将这一结果与我们的四个先前结果相结合,以计算我们的K(b)确定的全球加权平均值。计算遵循Codata的方法(MoHR和Taylor 2000 Rev. Mod.Mym.72 351),用于获得k(b)的加权平均值,该k(b)占该工作中测量数量之间的相关性的相关性,并在我们的四个先前的k确定中(b)。上帽的加权平均值(K(B))为1.3806484(28)×10(-23)J K-1,相对标准不确定性为2.0×10(-6)。通用气体常数的相应值为8.314459(17)J K-1mol(-1),相对标准不确定度为2.0×10(-6)。

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