The Molecular Fields of Carbon Dioxide and Nitrous Oxide
The Molecular Fields of Carbon Dioxide and Nitrous Oxide
复制标题
二氧化碳和一氧化二氮的分子场
DOI:
10.1098/rspa.1939.0162
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发表时间:
1939
期刊:
影响因子:
--
通讯作者:
T. Ibbs
中科院分区:
文献类型:
--
作者:
R. E. Bastick;H. R. Heath;T. Ibbs
Experiments show that the thermal separation produced in a mixture of two gases by a temperature gradient may generally be regarded as proportional to log ( T 1/ T 2) over a considerable range of ordinary temperature, T 1 being the absolute temperature of the hot side and T 2 that of the cold side. Thus the total difference in concentration in the mixture may be written Δλ = kt log ( T 1/ T 2), where the constant kt is the coefficient of thermal separation. The theoretical meaning of the constancy of kt (Chapman 1918) is that the unlike molecules may be regarded as point centres of repulsive force obeying an inverse power law. At lower temperatures there is a general tendency for kt to decrease gradually with temperature. The general expression for the experimental value of kt may be written kt = - dλ 1/ d log T = dλ 2/ d log T' where λ 1 is the proportion of the heavier gas, λ 2 the proportion of lighter gas, and λ 1 + λ 2 = 1. A peculiarity has been found in the measurements of thermal separation in mixtures containing carbon dioxide, in that kt changes from one definite value below about 145° C to a higher definite value above that temperature (Ibbs and Wakeman 1932). This led to the conclusion that there is a change in the nature of the molecular field of carbon dioxide from a “soft” molecule to a “harder” molecule, i.e. the behaviour above 145° C becomes more like that of a rigid elastic sphere. Measurements of the viscosity of carbon dioxide support this conclusion.