Some Thermodynamic Properties of Pure and Impure Nitrogen

1974 ◽  
Vol 52 (16) ◽  
pp. 1521-1531 ◽  
Author(s):  
J. Ancsin

Boiling points, freezing points, and vapor pressures (from 56 K to the normal boiling point) for pure and various doped N2 samples have been measured. The normal boiling points for N2 and N2 doped with 100 v.p.p.m. of O2, Ar, Kr, and CO impurities were found to be 77.3439 K, 77.3458 K, 77.3452 K, 77.3454 K, and 77.3444 K respectively. The triple points of the same samples are 63.14635 K, 63.1445 K, 63.14575 K, 63.1487 K, and 63.14675 K respectively. The values obtained for the heats of sublimation, vaporization, and fusion at the triple point of pure N2 were 6773.8, 6049.6, and 724.3 J/mole respectively and the above impurities changed these quantities by the amounts given in Tables 5 and 6.

2006 ◽  
Vol 248 (1) ◽  
pp. 70-77 ◽  
Author(s):  
Eleni Panteli ◽  
Epaminondas Voutsas ◽  
Kostis Magoulas ◽  
Dimitrios Tassios

It appeared that further experiments on the viscosity of air were desirable in order to discriminate between the results of F. A. Williams* and those of most previous observers, and to test his conclusion respecting the validity of Sutherland’s law of the variation of viscosity with temperature. It happened that this could be done easily and expeditiously in the laboratories of the Imperial College. Mr. R. S. Edwards, the author of the following paper, was in the midst of preparations for determining the viscosity of neon at a number of temperatures ranging from atmospheric temperature to the normal boiling point of sulphur, and at my suggestion diverted his attention to the behaviour of air at the same temperatures. It is true that this range (about 430 centi­grade degrees) is not so extensive as the thousand degrees covered by Williams’ experiments, but it includes all that region in which, according to Williams, the value of Sutherland’s constant displays the large increase upon which I have cast doubt. Edwards’ method of temperature control and estimation involves heating by the saturated vapour of selected substances of well-established boiling points, and would appear to be more reliable than the electrical heating, and particularly the temperature measurement by a single thermocouple, as employed by Williams. In the present experiments also, considerable variations of the pressure conditions have been made, with consistent results, thus proving the validity of the transpiration formula assumed. No such internal evidence of accuracy was provided in Williams’ experiments.


Metrologia ◽  
1970 ◽  
Vol 6 (1) ◽  
pp. 35-37 ◽  
Author(s):  
G T Furukawa ◽  
W G Saba ◽  
D M Sweger ◽  
H H Plumb

2002 ◽  
Vol 198 (1) ◽  
pp. 81-93 ◽  
Author(s):  
Epaminondas Voutsas ◽  
Maria Lampadariou ◽  
Kostis Magoulas ◽  
Dimitrios Tassios

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