scholarly journals The second virial coefficient of a gas of non-spherical molecules

Tables are given for the second virial coefficient and Joule-Thomson coefficient (at low pressures) of a gas whose molecules are non-polar, approximately cylindrical, and stiff. The tables cover the range of length/breadth ratio consistent with the last assumption. The tables can be used for the analysis of observed virial coefficients of gases whose molecules satisfy these assumptions, and give an estimate of the intermolecular forces between these molecules at any relative orientation. For small ratio of length to breadth the virial coefficient is nearly the same as that of a spherical molecule with certain mean values of the parameters defining the intermolecular field. This makes it possible to relate these mean parameters to the critical constants and to the parachor. The virial coefficients of nine gases are analysed. The data on seven hydrocarbons enable one to estimate the law of force between molecules of the lower non-polar hydrocarbons.

1967 ◽  
Vol 20 (9) ◽  
pp. 1789 ◽  
Author(s):  
GA Bottomley ◽  
TH Spurling

Second virial coefficients have been determined for carbon disulphide, methyl chloride, acetone, and methanol over the temperature range of 50-150� with some additional results at lower temperatures. Similar work has been conducted on the selected mixtures methyl chloride-carbon disulphide, methyl chloride-acetone, acetone-carbon disulphide, and methyl chloride-argon. Methanol, exceptionally, shows very significant third virial contributions in the sub-atmospheric pressure range. A comparison is made with recent models pertaining to molecular interactions between unlike molecules possessing dipolar and quadrupolar contributions to the intermolecular forces.


The second virial coefficients of binary mixtures of chloroform with methyl formate, n -propyl formate, methyl acetate, ethyl acetate and diethylamine have been measured in a ‘Boyle’s law apparatus’ at temperatures between 50 and 95 °C. The measured values are consistently higher than predicted by the theory of corresponding states, and a quantitative interpretation is proposed, based on the hypothesis that the esters and amine are partially dimerized and are involved in association with the chloroform by hydrogen bonding. A linear relation is shown to exist between the heats and entropies of association for the various mixtures, and the theoretical significance of this is discussed. There is some evidence that hydrogen bonds are formed through the alkoxyl oxygen by formate esters and through the carbonyl oxygen by acetate esters. The paper includes data on the second virial coefficient for the pure esters and for ethyl formate and methyl propionate.


2001 ◽  
Vol 66 (6) ◽  
pp. 833-854 ◽  
Author(s):  
Ivan Cibulka ◽  
Lubomír Hnědkovský ◽  
Květoslav Růžička

Values of adjustable parameters of the Bender equation of state evaluated for chloromethane, dichloromethane, trichloromethane, tetrachloromethane, and chlorobenzene from published experimental data are presented. Experimental data employed in the evaluation included the data on state behaviour (p-ρ-T) of fluid phases, vapour-liquid equilibrium data (saturated vapour pressures and orthobaric densities), second virial coefficients, and the coordinates of the gas-liquid critical point. The description of second virial coefficient by the equation of state is examined.


The prediction of the virial coefficients for particular intermolecular potentials is generally regarded as a difficult mathematical problem. Methods have only been available for the second and third coefficient and in fact only few calculations have been made for the latter. Here a new method of successive approximation is introduced which has enabled the fourth virial coefficient to be evaluated for the first time for the Lennard-Jones potential. It is particularly suitable for automatic computation and the values reported here have been obtained by the use of the EDSAC I. The method is applicable to other potentials and some values for these will be reported subsequently. The values obtained cannot yet be compared with any experimental results since these have not been measured, but they can be used in the meantime to obtain more accurate experimental values of the lower coefficients.


The second virial coefficients of some binary mixtures of organic vapours have been measured at temperatures between 50 and 120° C. Mixtures of n -hexane with chloroform and of n -hexane with diethyl ether show a linear variation of second virial coefficient with composition. This is shown to be in accordance with prediction from the principle of corresponding states. Mixtures of chloroform with diethyl ether show a linear variation at 120° C, but pronounced curvature at lower temperatures. This is interpreted quantitatively as being due to association by hydrogen bonding with an energy of 6020 cal/mole.


A general theory of the second virial coefficient of axially symmetric molecules is developed, the directional part of the intermolecular field being treated as a perturbationon the central-force part. The method is applicable to any type of intermolecular potential, particular models of directional interaction being obtained by suitable choices of parameters. Simple expressions are given for the second virial coefficient due to several types of directional force. The theory is illustrated by some calculations on the force field of carbon dioxide and its relation to the second virial coefficient and crystal data. These indicate that there is strong quadrupole interaction between carbon dioxide molecules.


1964 ◽  
Vol 17 (5) ◽  
pp. 501 ◽  
Author(s):  
GA Bottomley ◽  
TH Spurling

An unconventional apparatus, described in detail, determines, through a measured small volume increment, the temperature dependence of the second virial coefficient of a vapour without the necessity for isothermal expansion. Absolute pressure determinations are avoided by working differentially, vapour against nitrogen reference gas. Results for n-butane at 0-150� agree with established work.


The density of benzene vapour at about 70% saturation at 22 °C has been determined experimentally by the microbalance method using nitrogen as the comparison gas. The adsorption of the benzene vapour on the particular working parts of the two balances used in the work was determined in separate experiments, so that full correction of the density determinations for this influence was possible. The second virial coefficient of the vapour has been deduced at 22 °C and, from similar measurements, at 35 °C.


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