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A Determination of the Ratio of the Zinc Freezing Point to the Tin Freezing Point by Noise Thermometry

机译:噪声测温法测定锌凝固点与锡凝固点之比。

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A Johnson-noise thermometer (JNT) has been used with a quantized voltage noise source (QVNS), as a calculable reference to determine the ratio of temperatures near the Zn freezing point to those near the Sn freezing point. The temperatures are derived in a series of separate measurements comparing the synthesized noise power from the QVNS with that of Johnson noise from a known resistance. The synthesized noise power is digitally programed to match the thermal noise powers at both temperatures and provides the principle means of scaling the temperatures. This produces a relatively flat spectrum for the ratio of spectral noise densities, which is close to unity in the low-frequency limit. The data are analyzed as relative spectral ratios over the 4.8 to 450 kHz range averaged over a 3.2 kHz bandwidth. A three-parameter model is used to account for differences in time constants that are inherently temperature dependent. A drift effect of approximately −6 μK·K−1 per day is observed in the results, and an empirical correction is applied to yield a relative difference in temperature ratios of −11.5 ± 43 μK·K−1 with respect to the ratio of temperatures assigned on the International Temperature Scale of 1990 (ITS-90). When these noise thermometry results are combined with results from acoustic gas thermometry at temperatures near the Sn freezing point, a value of T − T 90 = 7 ± 30 mK for the Zn freezing point is derived.
机译:约翰逊噪声温度计(JNT)已与量化电压噪声源(QVNS)一起使用,作为可计算的参考,以确定Zn凝固点附近的温度与Sn凝固点附近的温度之比。通过一系列独立的测量得出温度,将QVNS的合成噪声功率与已知电阻的Johnson噪声功率进行比较。对合成噪声功率进行数字编程,以匹配两个温度下的热噪声功率,并提供了缩放温度的基本方法。对于频谱噪声密度的比率,这将产生一个相对平坦的频谱,在低频范围内接近于1。将数据分析为4.8至450 kHz范围内的相对频谱比,将其相对于3.2 kHz带宽平均。三参数模型用于解决固有取决于温度的时间常数的差异。结果中观察到每天大约-6μK·K -1 的漂移效应,并且进行了经验校正,得出温度比的相对差为-11.5±43μK·K <关于1990年国际温度标度(ITS-90)分配的温度比的sup> -1 。当将这些噪声测温结果与在Sn凝固点附近的温度下的声气测温结果相结合时,可得出Zn凝固点的T-T 90 = 7±30 mK。

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