Prediction of Solid + Liquid Equilibrium Diagrams for Binary Mixtures Forming Solid Solutions with an Extremum

1982 ◽  
Vol 19 ◽  
Author(s):  
Witold Brostow ◽  
M. Antonieta Macip

ABSTRACTConvenient methods of correlation and prediction of S+L diagrams exist only for systems forming eutectics. To deal with solid solutions, we have adopted the model of strictly regular solutions of Guggenheim [3–5]. Our key assumption is that values of the Gibbs function of interchange w are different in the two coexisting phases: wS and wL. The assumption is based on the fact that the average interatomic distances R are also different, and this affects the averages of the interatomic (or intermolecular) potentials. The input parameters are enthalpies and temperatures of melting of pure components and any pair of experimental points on the diagram. For a number of binary alloy systems the agreement with the experiment is good. Since we believe in the basic unity of materials (see Chap. 1 in [7]), calcuations have also been made for organic mixtures, again with good results.

2016 ◽  
Vol 427 ◽  
pp. 1-8 ◽  
Author(s):  
Laslo A.D. Boros ◽  
Marta L.S. Batista ◽  
J.A.P. Coutinho ◽  
M.A. Krähenbühl ◽  
Antonio J.A. Meirelles ◽  
...  

2021 ◽  
pp. 113327
Author(s):  
Ericsem Pereira ◽  
Débora Tamires Vitor Pereira ◽  
Antonio J.A. Meirelles ◽  
Guilherme J. Maximo

1983 ◽  
Vol 22 ◽  
Author(s):  
William B. Streett ◽  
Andreas Heintz ◽  
Paulette Clancy ◽  
Dhanraj Chokappa

ABSTRACTExperimental measurements have been carried out to determine the compositions of coexisting gas and liquid phases for binary mixtures of hydrogen with the following substances as the second component: nitrogen, carbon monoxide, argon, methane, ethylene, ethane and carbon dioxide. For most of these mixtures the entire region of gas-liquid equilibrium has been explored for the first time. This region is bounded in pressure-temperature space by the vapor-pressure curve of the heavy component, the gas-liquid critical line (where gas and liquid phases become identical) and the 3-phase region solid-liquid-gas. In all of the systems described here the latter two lines intersect to form a critical end point. The general qualitative features of these phase diagrams are described, and compared to those of helium mixtures studied earlier.


2014 ◽  
Vol 366 ◽  
pp. 88-98 ◽  
Author(s):  
Guilherme J. Maximo ◽  
Natália D.D. Carareto ◽  
Mariana C. Costa ◽  
Adenilson O. dos Santos ◽  
Lisandro P. Cardoso ◽  
...  

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