1965
DOI: 10.6028/jres.069a.002
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Application of precise heat-capacity data to the analysis of the temperature intervals of the NBS (1955) and the International Practical Temperature Scales in the region of 90 °K

Abstract: A method is presented for analyz in g t he te mperature in terva ls of the ~BS (1955) temperature scale a nd the International Practical Temperature Scale (IPTS) . Values of d1'/dR as a fun ction of resista nce a re d erived from equations of dQ / dR a nd dQ /dT, obtained from precise beat-capacity data (better t ha n ± 0.02 p ercent) by the method of lea st squa res .An adjusted t emperature scale is obtain ed by integration of the values of dT/dR relative to a referen ce t empera tu re a nd the correspondi… Show more

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Cited by 10 publications
(3 citation statements)
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“…Heat-capacity determinations using resistance thermometry are dependent on the dR/dT or essentially the "size of the degree" of the temperature scale. Heat-capacity results, obtained using the NBS-1955 and the IPTS, exhibit reproducible anomalies as large as 0.2 percent that are attributable to deviations of these temperature scales from the thermodynamic scale [47]. Barber 273°K which is as closely related to the thermodynamic scale as the present knowledge permits [85,7].…”
Section: General Appraisal Of Low-temperature Heat-capacity Measurementsmentioning
confidence: 98%
“…Heat-capacity determinations using resistance thermometry are dependent on the dR/dT or essentially the "size of the degree" of the temperature scale. Heat-capacity results, obtained using the NBS-1955 and the IPTS, exhibit reproducible anomalies as large as 0.2 percent that are attributable to deviations of these temperature scales from the thermodynamic scale [47]. Barber 273°K which is as closely related to the thermodynamic scale as the present knowledge permits [85,7].…”
Section: General Appraisal Of Low-temperature Heat-capacity Measurementsmentioning
confidence: 98%
“…The total weight of the loaded cell was about 390 g. Class S-2 calibrated weights designated NBS 3246 were used. The sample weight was adjusted for air buoyancy using 1.123 g/cm 3 as the density of diethyl phthal-) ate, 8.40 g/cm 3 as the density of the brass weights, and 0.00120 g/cm 3 as the density of air.…”
Section: Preparation Of Samplementioning
confidence: 99%
“…For each determination on the empty calorimeter, the initial temperature, final temperature, and energy increment were fitted to a polynomial by the method of Furukawa and Reilly (5), in such a manner as to minimize the difference between Qobsd, the experimental energy increment, and Qcalcd, the energy increment calculated from the polynomial for the temperature range of the experiment. The resulting equation for the heat capacity of the empty calorimeter was Ce = 15.964705 + 6.207663 x 10% -5.965945 1 (1) where Ce is in joules per degree and t is in °C.…”
Section: Resultsmentioning
confidence: 99%