1956
DOI: 10.1080/14786435608238162
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LXXXVII. The specific heats of cadmium and mercury

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Cited by 47 publications
(4 citation statements)
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“…We follow NBS 270-4 in taking ß,°= 0, AH,0 = 0, and S°= 18.17 cal K-1 mol-1 for Hg(liq) at 298 K. This entropy is consistent with the heat capacities of Busey and Giauque30 and Smith and Wolcott. 31 We also note that Douglas, Ball, and Ginnings32 have measured (Hr -H273) for Hg(liq) by a "drop" method over the range 0-450°C.…”
Section: Elementary Mercurymentioning
confidence: 78%
“…We follow NBS 270-4 in taking ß,°= 0, AH,0 = 0, and S°= 18.17 cal K-1 mol-1 for Hg(liq) at 298 K. This entropy is consistent with the heat capacities of Busey and Giauque30 and Smith and Wolcott. 31 We also note that Douglas, Ball, and Ginnings32 have measured (Hr -H273) for Hg(liq) by a "drop" method over the range 0-450°C.…”
Section: Elementary Mercurymentioning
confidence: 78%
“…Durch Vergleich des Ohmschen Gesetzes (j)=a@ mit den Ergebnissen (20) und (23) Der Grenzwert des Pt ergibt sich nach Ausffihrung der Summation fiber die Kennzablen der Zust/inde und q zu In dieser Nfiherung erhalten wir den gleichen Wert wie in der klassischen Theorie.…”
Section: Die Komponenten Des Leiff~ihigkeitstensorsunclassified
“…Wir machen den Vergleich mit den Messungen an Cd bei der Temperatur T=78 ~ Die zur numerischen Berechnung n6tigen Gr6Ben sind: Fermienergie (= 1,21 • 10-11 erg, die aus der spezifischen Wftrme [20] berechnet ist, Schallgeschwindigkeit q = 3,74 x 105 cm sec-1 die sich aus elastischen Konstanten [21] …”
Section: Vergleich Mit Dem Experimentsunclassified
“…The heat capacity C(T) of solid mercury has been studied experimentally in sufficient details [1,2,[6][7][8][9][10][11][12][13][14]. However, the empirical data on the thermal expansion coefficient (in what follows, we will con sider the volumetric coefficient (VTEC) ο(T) = (1/V) ) are insufficient, in particular, at low ∂V ∂T ⎝ ⎠ ⎛ ⎞ P temperatures [1,2,12,[15][16][17][18][19].…”
Section: Introductionmentioning
confidence: 99%