1969
DOI: 10.1088/0026-1394/5/4/001
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Investigation of the Resistance-Temperature Properties of Platinum for Resistance Thermometry over the Range from 14 K to 90 K

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Cited by 5 publications
(3 citation statements)
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“…2 and 3, where the baseline in all cases is the mean temperature computed for the eight thermometers of Fig. 2a If this, we think highly plausible, assumption of uncertainties in the originally assigned values of W (100 "C) is valid, it is evident that the IPTS-68 is more reproducible in the range 90 K to 273 K than On the basis of these forty-eight thermometers the IPTS-68 is not reproducible to better than * 3 mK in 4 The large apparent deviations of the four thermometers of Fig. 3a are not real, but arise from inconsistencies in transferring their calibrations to our baseline.…”
Section: Preston-thomas and Bedfordmentioning
confidence: 82%
“…2 and 3, where the baseline in all cases is the mean temperature computed for the eight thermometers of Fig. 2a If this, we think highly plausible, assumption of uncertainties in the originally assigned values of W (100 "C) is valid, it is evident that the IPTS-68 is more reproducible in the range 90 K to 273 K than On the basis of these forty-eight thermometers the IPTS-68 is not reproducible to better than * 3 mK in 4 The large apparent deviations of the four thermometers of Fig. 3a are not real, but arise from inconsistencies in transferring their calibrations to our baseline.…”
Section: Preston-thomas and Bedfordmentioning
confidence: 82%
“…The thermometers that were investigated by Hoge and Brickwedde showed a spread of 7 mK between 190 and 0 C, and spread of 1.3 mK between 0 and 100 C. The six thermometers measured between 100 and 444 C had a maximum spread of 12 mK. Data which would indicate the spread of interpolated values of temperature on the IPTS 68 below C due to the variations in presently acceptable platinum wire is sparse and inadequate [11,36,44]. On the basis of existing data, Bedford and Ma [9] estimated that the IPTS-68 is reproducible to 3 mK between 14 and 20 K, 1 mK between 20 and 54 K, it 2 mK between 54 and 90 K, and 5 mK between 90 and 273 K. It should be pointed out that, in addition to unaccounted for variations in the platinum wire, a spread in the temperature values may also arise from incomplete definitions of the materials that define fixed points (e.g., their isotopic composition).…”
Section: *3 Errors Of Temperature Determinationsmentioning
confidence: 99%
“…Non-uniqueness resulting from applying our deviation function [Eq. (7)] to the resistance ratio differences among nine thermometers from references [3] and [4]. The coefficients of the deviation functions were calculated from the resistance ratio differences a t those temperatures marked with asterisks.…”
mentioning
confidence: 99%