THE FREE ENERGY, HEAT CONTENT AND ENTROPY OF IODINE MONOCHLORIDE

1932 ◽  
Vol 54 (6) ◽  
pp. 2247-2256 ◽  
Author(s):  
John McMorris ◽  
Don M. Yost
1932 ◽  
Vol 24 (12) ◽  
pp. 1388-1391 ◽  
Author(s):  
J. B. Austin
Keyword(s):  

The partial molar heat content, entropy and free energy of benzene in solutions of diphenyl in benzene have been determined by measurement of the partial pressures of benzene over the solu-­ tions. The whole composition range has been covered (as far as the solubility of diphenyl will allow), at temperatures from 30 to 80° C. A check on the accuracy of the experimental method has been made by measuring the vapour pressure of pure benzene over this temperature range, and good agreement has been found with recent values reported in the literature. The calculation of the thermodynamic functions from the vapour pressures requires a knowledge of the compressibility of benzene vapour. An experimental method has been devised for determining the gas imperfections of vapours, and using this the second and third virial coefficients of benzene vapour at various temperatures have been obtained. The variation of the thermodynamic functions of benzene with the composition of the solutions has been compared with that to be expected on the basis of recent statistical theories. It is found that whereas the non-ideal partial molar free energy can be accounted for almost exactly by the theo­ retical expression, the separate heat contents and entropies show some deviations. It is suggested that these deviations arise from slight changes in molecular packing as the composition is varied. The activities of benzene and diphenyl in saturated solutions at 30 to 60° C have been obtained from the vapour pressures of saturated solutions at these temperatures. These lead to values for the latent heat of fusion of diphenyl in agreement with the calorimetric value. The yapour pressure of saturated solutions is discussed.


In Part I of this series were described measurements of the free energy and heat content of hydrogen chloride in a series of water-alcohol mixtures. It appeared to be very desirable to find if the behaviour shown by hydrogen chloride is typical of that of strong electrolytes in general. For this purpose an attempt was made in the first place to determine the free energies of lithium chloride in these solvents, using amalgam electrodes. Preliminary measurements showed that even Under rigidly air-free conditions reproducible values of the electromotive forces of cells containing lithium amalgams could not be obtained in alcohol solutions. Similar experiences with sodium amalgams have been reported from the Balliol College Laboratory, while Scatchard has also experienced similar difficulties with calcium amalgams. It appeared that zinc chloride might be suitable, for when proper precautions are taken for the with zinc amalgam in aqueous solutions. The conductivities show that zinc chloride is a strong electrolyte in aqueous solution, and although several investigators have found that their product hydrolysed to give turbid solutions in water, we had no difficulty in obtaining a salt which gave perfectly clear solutions at all dilutions. The conductivity measurements of Getman and Gibbons, which show that in alcoholic solution zinc chloride is an extremely weak electrolyte, escaped our notice at the beginning of this work. But although on this account the behaviour of zinc chloride does not extend our knowledge of the properties of completely ionised substances in mixed solvents, it has proved to be an interesting case showing in the range of solvents investigated the transition from a strong to an exceedingly weak electrolyte. The free energies were determined by measuring the electromotive force of cells of the type Zn 1 percent. amalgam | ZnCl 2 , ( m ) Alcohol, N mols. per cent. AgCl( s ) | Ag The free energy change in the cell reaction, viz., Zn (Hg) + 2AgCl( s ) = ZnCl 2 ( m , N) + 2Ag, is given by ∆F = - 2 EF = - 46148E calories, where E is the electromotive force and F the electrochemical equivalent. The electromotive forces were determined in solvents containing 0, 25, 50, 90 and 100 mols. per cent, alcohol, each for a range of salt concentrations from about m = 0⋅01 to m = 1, at 15 ± 0⋅02°. It was originally intended to make a similar series of measurements also at 25°, in order to evaluate the heat content changes, but the reproducibility of the results in solutions containing large proportions of alcohol did not warrant this extension.


The two acid dissociation constants of the ethylene diammonium ion and the hexamethylene diammonium ion in water have been determined, using an e.m.f. method, from 0 to 60° C. Measurements have been made at several ionic strengths to allow thermodynamic dissociation constants to be derived, and from these the free energy, heat content, entropy and heat capacity changes accompanying the dissociations have been computed. These quantities are discussed in relation to the size of the diamine molecule, and orientation of solvent molecules by the ionic charges. It is concluded that the range over which a single ionic charge causes a significant change in the structure of liquid water is about 5 Å.


The increase in heat content attending the isobaric formation of liquid mixtures of acetone and methyl iodide in varying proportions has been determined calorimetrically in the temperature range 253 to 308 °K. The corresponding change in free energy has been measured from analyses of the mixed vapour at equilibrium with the mixed liquids. By difference, the change in entropy associated with the mixing has been found. Most of this derives, as is usual, from the randomness of the mixture, but there is a relatively small residuum (the so-called excess entropy of mixing) which is found to vary in an unusual way with respect to the composition.


1955 ◽  
Vol 28 (3) ◽  
pp. 838-849
Author(s):  
G. L. Starobinets ◽  
Kh M. Aleksandrovich

Abstract 1. The swelling of vulcanizates of natural rubber and sodium-butadiene rubber in the saturated vapors of binary systems of benzene and low-molecular alcohols (from methyl to butyl) at 20° and 50° C was studied in the entire range of composition of binary solutions. 2. The general form of the curves of isothermic equilibrium between the swollen polymer and binary solution were found to conform to Konovalov's law. 3. The absorption of a binary solution by both polymers has a very pronounced selective character. The selectivity of absorption of the solution is more pronounced, the greater is the density of energy of cohesion of the alcohol. In natural rubber, the capacity of selective absorption is more pronounced than in sodium-butadiene rubber. This is probably due to the larger concentration of oxidized groups in natural rubber. 4. The changes of the free energy, the heat content, and entropy for the passage of one gram-mole of alcohol from an infinitely dilute solution into the polymer were calculated from the experimental data. These calculations indicate that the reaction of the alcohol molecules with the polar groups of the polymer is dipole-dipole. 5. The passage from pure benzene to a swollen polymer of any particular composition is characterized by a large increase of entropy in comparison with the passage to a binary solution of the same composition. The relation in alcohol is the reverse. The increase of the entropy of benzene can serve as a measure of the elasticity of the polymer chains. A decrease of the entropy of alcohols indicates the content of free polar groups in the polymer phase. 6. The values of the partial heat content of the low-molecular components are positive; consequently, the decrease of free energy during their sorption by the polymer is due exclusively to an increase of entropy.


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