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Carbon continued high-temperature behaviour

The present paper gives an overview of results on high-pressure phase equilibria in the ternary system carbon dioxide-water-1-propanol, which has been investigated at temperatures between 288 and 333 K and pressures up to 16 MPa. Furthermore, pressure-temperature data on critical lines, which bound the region where multiphase equilibria are oberserved were taken. This study continues the series of previous investigations on ternary systems with the polar solvents acetone [2], isopropanol [3] and propionic add [4], A classification of the different types of phase behaviour and thermodynamic methods to model the complex phase behaviour with cubic equations of state are discussed. [Pg.241]

The isotherm EFGH at 21.5 C shows a similar behaviour except that now the liquefication commences at a higher pressure and the horizontal portion FG, representing decrease in volume, becomes smaller. At still higher temperatures, the horizontal portion of the curve becomes shorter and shorter until at 31.1 C it reduces just to a point (represented by X). At this temperature, therefore, the gas passes into liquid state imperceptibly. Above 31.1 C, the isotherm is continuous. There is no evidence of liquefaction at all. Andrews concluded that if the temperature of carbon dioxide is above 31.1 C, it cannot be- liquefied, no matter how high the pressure may be. He called 31.1 C as the critical temperature of carbon dioxide. Since then, other gases have been... [Pg.135]


See other pages where Carbon continued high-temperature behaviour is mentioned: [Pg.568]    [Pg.27]    [Pg.175]    [Pg.68]    [Pg.87]    [Pg.264]    [Pg.491]    [Pg.502]    [Pg.99]    [Pg.2]    [Pg.449]    [Pg.128]   
See also in sourсe #XX -- [ Pg.6 , Pg.7 , Pg.18 ]

See also in sourсe #XX -- [ Pg.6 , Pg.7 , Pg.18 ]




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