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Binary liquid mixture

Contact angle will vary with liquid composition, often in a regular way as illustrated in Fig. X-13 (see also Ref. 136). Li, Ng, and Neumann have studied the contact angles of binary liquid mixtures on teflon and found that the equation of state that describes... [Pg.370]

The discussion so far has been confined to systems in which the solute species are dilute, so that adsorption was not accompanied by any significant change in the activity of the solvent. In the case of adsorption from binary liquid mixtures, where the complete range of concentration, from pure liquid A to pure liquid B, is available, a more elaborate analysis is needed. The terms solute and solvent are no longer meaningful, but it is nonetheless convenient to cast the equations around one of the components, arbitrarily designated here as component 2. [Pg.406]

Fig. XI-11. Relation of adsorption from binary liquid mixtures to the separate vapor pressure adsorption isotherms, system ethanol-benzene-charcoal (n) separate mixed-vapor isotherms (b) calculated and observed adsorption from liquid mixtures. (From Ref. 143.)... Fig. XI-11. Relation of adsorption from binary liquid mixtures to the separate vapor pressure adsorption isotherms, system ethanol-benzene-charcoal (n) separate mixed-vapor isotherms (b) calculated and observed adsorption from liquid mixtures. (From Ref. 143.)...
Distillation, extractive distillation, liquid-liquid extraction and absorption are all techniques used to separate binary and multicomponent mixtures of liquids and vapors. Reference 121 examines approaches to determine optimum process sequences for separating components from a mixture, primarily by distillation. [Pg.1]

Relative volatility is the volatility separation factor in a vapor-liquid system, i.e., the volatility of one component divided by the volatility of the other. It is the tendency for one component in a liquid mixture to separate upon distillation from the other. The term is expressed as fhe ratio of vapor pressure of the more volatile to the less volatile in the liquid mixture, and therefore g is always equal to 1.0 or greater, g means the relationship of the more volatile or low boiler to the less volatile or high boiler at a constant specific temperature. The greater the value of a, the easier will be the desired separation. Relative volatility can be calculated between any two components in a mixture, binary or multicomponent. One of the substances is chosen as the reference to which the other component is compared. [Pg.22]

Van Stralen, S. J. D., Heat Transfer to Boiling Binary Liquid Mixtures, Part 1, British Chem. ng.,Jan. (1959) p. 8. [Pg.288]

Of great practical importance are the liquid solutions produced by mixing together pure liquids. The simplest type comprises the binary liquid mixtures, such as mixtures of water and alcohol. [Pg.380]

The vapour-pressure curves of binary liquid mixtures have been considered from another point of view by Dolezalek (Zeitscher. physik. Chem. 64, 727, (1908)), who starts out with the very simple assumption that the partial pressure of each component is proportional to its concentration in the liquid phase, provided no chemical change occurs when the liquids are mixed, and that neither component is polymerised in the liquid state. Thus ... [Pg.402]

In considering the thermal magnitudes of importance in the study of binary liquid mixtures, we shall confine our attention to the simplest case, in which it can be assumed that ... [Pg.404]

Such a system is formed, for example, by a binary liquid mixture in contact with its vapour, or a mixed crystal in contact with its melt. [Pg.413]

If a binary liquid mixture is contained in a cylinder under a piston, and the latter slowly raised, evaporation proceeds, and the quantities and compositions of liquid and vapour gradually change. According to the conditions, the evaporation may proceed at constant temperature (p variable), or at constant pressure (T variable). The latter case usually occurs in practice (cf. 163-164). [Pg.415]

Since Ag is a function of pressure, it follows that, under certain conditions, a change in pressure may produce immiscibility in a completely miscible system, or, conversely, such a change may produce complete miscibility in a partially immiscible system. The effect of pressure on miscibility in binary liquid mixtures is closely connected with the volume change on mixing, as indicated by the exact relation... [Pg.184]

In the previous sections, we indicated how, under certain conditions, pressure may be used to induce immiscibility in liquid and gaseous binary mixtures which at normal pressures are completely miscible. We now want to consider how the introduction of a third component can bring about immiscibility in a binary liquid that is completely miscible in the absence of the third component. Specifically, we are concerned with the case where the added component is a gas in this case, elevated pressures are required in order to dissolve an appreciable amount of the added component in the binary liquid solvent. For the situation to be discussed, it should be clear that phase instability is not a consequence of the effect of pressure on the chemical potentials, as was the case in the previous sections, but results instead from the presence of an additional component which affects the chemical potentials of the components to be separated. High pressure enters into our discussion only indirectly, because we want to use a highly volatile substance for the additional component. [Pg.194]

We consider a binary liquid mixture of components 1 and 3 to be consistent with our previous notation, we reserve the subscript 2 for the gaseous component. Components 1 and 3 are completely miscible at room temperature the (upper) critical solution temperature Tc is far below room temperature, as indicated by the lower curve in Fig. 27. Suppose now that we dissolve a small amount of component 2 in the binary mixture what happens to the critical solution temperature This question was considered by Prigogine (P14), who assumed that for any binary pair which can be formed from the three components 1, 2 and 3, the excess Gibbs energy (symmetric convention) is given by... [Pg.195]

Bomlia, C.F. and Perry, C.H. Trans. Am. lust. Chem. Eng. 37 (1941.i 685. Heat transmission to boiling binary liquid mixtures. [Pg.564]

To express the composition of the vapor in equilibrium with the liquid phase of a binary liquid mixture, we first note that the definition of partial pressure (PA = xAP for component A) and Dalton s law (P = PA + PB) allow us to express the composition of the vapor of a mixture of liquids A and B in terms of the partial pressures of the components ... [Pg.460]

The normal boiling point of a binary liquid mixture is the temperature at which the total vapor pressure is equal to 1 atm. If we were to heat a sample of pure benzene at a constant pressure of 1 atm, it would boil at 80.1°C. Similarly, pure toluene boils at 110.6°C. Because, at a given temperature, the vapor pressure of a mixture of benzene and toluene is intermediate between that of toluene and benzene, the boiling point of the mixture will be intermediate between that of the two pure liquids. In Fig. 8.37, which is called a temperature-composition diagram, the lower curve shows how the normal boiling point of the mixture varies with the composition. [Pg.461]

Frank, H. S. Evans, M. W. (1945). Entropy in binary liquid mixtures partial molal entropy in dilute solutions structure and thermodynamics in aqueous electrolytes. Journal of Chemical Physics, 13, 507-32. [Pg.52]

Liquid-Fluid Equilibria Nearly all binary liquid-fluid phase diagrams can be conveniently placed in one of six classes (Prausnitz, Licntenthaler, and de Azevedo, Molecular Thermodynamics of Fluid Phase Blquilibria, 3d ed., Prentice-Hall, Upper Saddle River, N.J., 1998). Two-phase regions are represented by an area and three-phase regions by a line. In class I, the two components are completely miscible, and a single critical mixture curve connects their criticsu points. Other classes may include intersections between three phase lines and critical curves. For a ternary wstem, the slopes of the tie lines (distribution coefficients) and the size of the two-phase region can vary significantly with pressure as well as temperature due to the compressibility of the solvent. [Pg.15]

Consider the situation where a sa le is incompletely resolved on two different liquid phases and the cosponents unseparated on each phase are not the same. The natural conclusion would be that a complete separation could probably be obtained if the two phases were combined- in appropriate proportions. Given the separations on the two pure liquids how can one calculate the exact cosposltion of a binary liquid phase mixture that will provide coBq>lete resolution of the sa >le A method for this purpose, based on the theory of diachoric solutions, was developed by Purnell and Laub [414-417]. It is commonly known as the windqy diagras method and has been applied with success to a number of practical problems. [Pg.621]

Gelb, L. D. Gubbins, K. E., Studies of binary liquid mixtures in cylindrical pores phase separation, wetting and finite-size effects from Monte Carlo simulations, Physica A 1997, 244, 112-123... [Pg.386]

Tewari, Y.B., Martire, D.E., Wasik, S.P., Miller, M.M. (1982a) Aqueous solubilities and octanol-water partition coefficients of binary liquid mixtures of organic compounds at 25°C. J. Solution Chem. 11, 435 445. [Pg.403]

We report in Table VII the signs of the excess functions reported in the literature for eight binary liquid mixtures of simple molecules the corresponding values of 8 and p for each mixture are given (first component = reference component A) as well as the temperature and TAA. These values of 8 andp have been deduced from Tables V and VI, and the reference component has been chosen in such a way that all the <5 s are positive. [Pg.138]

LS measurements on binary liquid mixtures have been directed primarily as a means of obtaining fundamental thermodynamic information such as chemical potentials and the excess mixing functions. Although molecular weights could in fact be derived from some published data, this has largely not been done by the authors, since such an exercise on substances of known molecular weight would have been subsidiary to the main purpose of their studies. [Pg.182]

Jenning, V, Mader, K. and Gohla, S. H., Solid lipid nanoparticles (SLN) based on binary mixtures of liquid and solid lipids a H-NMR study. Int. J. Pharm., 205, 15-21, 2000. [Pg.14]

Bjola, B.S., Siddiqi, M.A., and Svejda, P. Excess enthalpies of binary liquid mixtures of y-butyrolactone + benzene. + toluene, -t ethylbenzene, and -t carbon tetrachloride, and excess volume of the y-butyrolactone + carbon tetrachloride liquid mixture, / Chem. Eng. Data, 46(5) 1167-1171, 2001. [Pg.1633]


See other pages where Binary liquid mixture is mentioned: [Pg.371]    [Pg.132]    [Pg.403]    [Pg.184]    [Pg.185]    [Pg.195]    [Pg.430]    [Pg.430]    [Pg.459]    [Pg.459]    [Pg.460]    [Pg.460]    [Pg.470]    [Pg.1039]    [Pg.184]    [Pg.184]    [Pg.144]    [Pg.251]    [Pg.464]    [Pg.545]    [Pg.219]    [Pg.226]   
See also in sourсe #XX -- [ Pg.381 ]




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