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Mixtures temperature diagrams

Use the data given in Figure 2-20 to prepare a pressure-temperature diagram of a 52.4 weight percent n-heptane in n-pentane mixture. [Pg.86]

Phase Diagram for a Pure Substance — Use of Phase Diagrams — Vapor Pressure of a Pure Substance Pressure-Volume Diagram for a Pure Substance -Density-Temperature Diagram for a Pure Substance Two-Component Mixtures 61... [Pg.554]

To test the predictions, experiments were carried out at the Delft University of Technology (TUD) (Ballard et al., 2001). In CSMGem, the pressure versus temperature phase diagram was generated using the model and then confirmed by experimental data. Figure 5.19 is the pressure versus temperature diagram for a 30/70 mixture of ethane and propane in contact with excess water. [Pg.304]

If a liquid is in equilibrum with air, a part of this liquid is in the vaporous state and shows a temperature-dependent partial pressure. At the boiling point, the partial pressure equals the pressure of the ambient air. The partial pressure versus temperature diagram is very close to an exponential shape (Fig. 1.1). LEL and UEL, as volumetric values, correspond to partial pressures Plel and Puel- And these values define - on the temperature axis - two points, the LEP (Lower Explosive Point) and the UEP (Upper Explosive Point), which say the same as LEL and UEL below LEP and above UEP, an explosive mixture cannot be formed. [Pg.4]

As a final case, figure 3A.2 shows the pressure-temperature diagram (phase envelope) for the mixture containing 40.23% H2S, 9.88% COz, and 49.89% CH4, which is the mixture studied by Ng et al. (1985.) The data points on the plot are their data. [Pg.91]

Figure 1.14.4. Phase diagram for the solubility ot sugar in water. Note that when we were drawing a phase diagram for a pure substance, water or dry ice, the parameters that were varied were temperature and pressure. In this diagram, however, the phase diagram for a mixture, temperature and composition are the parameters being varied. Pressure is assumed to be constant. Figure 1.14.4. Phase diagram for the solubility ot sugar in water. Note that when we were drawing a phase diagram for a pure substance, water or dry ice, the parameters that were varied were temperature and pressure. In this diagram, however, the phase diagram for a mixture, temperature and composition are the parameters being varied. Pressure is assumed to be constant.
Figure 3 The composition-temperature diagram for pure poly-olefins showing UCST (upper critical solution temperature) and LCST (lower critical solution temperature) behaviour (because of the nature of this mixture, the UCST cannot be observed and therefore is dotted)... Figure 3 The composition-temperature diagram for pure poly-olefins showing UCST (upper critical solution temperature) and LCST (lower critical solution temperature) behaviour (because of the nature of this mixture, the UCST cannot be observed and therefore is dotted)...
Figure 3.2 Generic pressure-temperature diagram for binary mixtures of methane and ethane (i) pure methane (black line), (ii) I5mol% ethane (red lines), (iii) 5()mol% ethane (green lines), (iv) 70mol% ethane (blue lines), and (v) pure ethane (violet line). The solid lines and filled symbols denote the bubble point curves (saturated liquid), and the dashed lines and open symbols denote the dew point curves (saturated vapor). Data taken from RT Ellington et al.. Pap. Symp. Thermophys. Prop. 1, 180 (1959). Figure 3.2 Generic pressure-temperature diagram for binary mixtures of methane and ethane (i) pure methane (black line), (ii) I5mol% ethane (red lines), (iii) 5()mol% ethane (green lines), (iv) 70mol% ethane (blue lines), and (v) pure ethane (violet line). The solid lines and filled symbols denote the bubble point curves (saturated liquid), and the dashed lines and open symbols denote the dew point curves (saturated vapor). Data taken from RT Ellington et al.. Pap. Symp. Thermophys. Prop. 1, 180 (1959).
A schematic of a pressure-temperature diagram for a fixed composition mixture is shown in Figure 2.1. The phase representation of a mixture on a P P diagram is bivariant rather than univariant as in the case of a pure-component vapor pressure curve. At temperature Tj and pressure Pj, represented by point A, the mixture is... [Pg.75]

Takahashi, T., 320, 330, 331 Tea decaffeination plant, 7 Temperature-entropy diagram, 138 Temperature rising elution fractionation (TREF), 197, 202-203 Ternary mixtures, phase diagrams, 71-84 Testosterone, 340 Tetracyclic steroids, 293 Thermodynamic modeling, 99-134 Thies, M. C., 88-90... [Pg.511]

Concentration-Temperature Diagram.—In this diagram the temperatures are taken as the abscissae, and the composition of the solution, expressed in atoms of chlorine to one atom of iodine, is represented by the ordinates. In the diagram, A represents the melting-point of pure iodine, 114°. If chlorine is added to the system, a solution of chlorine in liquid iodine is obtained, and the temperature at which solid iodine is in equilibrium with the liquid solution will be all the lower the greater the concentration of the chlorine. We therefore obtain the curve ABF, which represents the composition of the solution with which solid iodine is in equilibrium at different temperatures. This curve can be followed down to 0°, but at temperatures below 7 9 (B) it represents metastable equilibria. At B iodine monochloride can be formed, and if present the system becomes invariant B is therefore a quadruple point at which the four phases, iodine, iodine monochloride, solution, and vapour, can co-exist. Continued withdrawal of heat at this point will therefore lead to the complete solidification of the solution to a mixture or conglomerate of iodine and iodine monochloride, while the temperature remains constant during the process. B is the eutectic point for iodine and iodine monochloride. [Pg.195]

Fig. 4 Concentration-Temperature diagram of mixture of two LCs (PAA-PAP), reproduced from E.C. HSU and J.F. Johnson, Mol. Cryst Liq. Cryst 20.177-183 (1973) (with permission Gordon and Breach). Fig. 4 Concentration-Temperature diagram of mixture of two LCs (PAA-PAP), reproduced from E.C. HSU and J.F. Johnson, Mol. Cryst Liq. Cryst 20.177-183 (1973) (with permission Gordon and Breach).
Figure 9.8 Pressure-temperature diagram for the alkane(l)-aromatic(2) mixture in Figures 9.4-9.7. Solid lines are pure vapor-pressure curves, ending at pure critical points (filled circles). Dashed line is the mixture critical line. Dash-dot lines are liquid constant-composition lines small dashed lines are vapor constant-composition lines. Filled square at A is a vapor-liquid equilibrium point it occurs at 14.5 bar, 386.7 K, Xj = 0.25, t/j = 0.75. Figure 9.8 Pressure-temperature diagram for the alkane(l)-aromatic(2) mixture in Figures 9.4-9.7. Solid lines are pure vapor-pressure curves, ending at pure critical points (filled circles). Dashed line is the mixture critical line. Dash-dot lines are liquid constant-composition lines small dashed lines are vapor constant-composition lines. Filled square at A is a vapor-liquid equilibrium point it occurs at 14.5 bar, 386.7 K, Xj = 0.25, t/j = 0.75.
Make reasonable assumptions. By considering the state of the system and the nature of its components, we can introduce sensible approximations that may vastly simplify the analysis but do little harm to the accuracy of the calculation. A consideration of the state would include identification of the phases present (solid, liquid, gas), estimates for temperature and pressure, and rough estimates for the composition. (For example, is a mixture dominated by one component or are any components present in very small amounts ). In general, it is helpful to locate known state points on phase diagrams, or at least to find where a mixture temperature lies relative to the pure-component melting and critical temperatures. By nature of the components we mean the kinds of intermolecular forces, such as simple van der Waals interactions, hydro-... [Pg.468]

Figure 2 Pressure-temperature diagram of a propane-oxygen mixture. Figure 2 Pressure-temperature diagram of a propane-oxygen mixture.
If the pressure is not equal to the system pressure p, the calculation has to be repeated. A better estimation of the temperature is found by plotting the values T and p in a vapor pressure/temperature diagram and drawing a hne parallel to the vapor pressure cmves of the pure substances of the mixture at hand. After a few iterations the following condition will be met ... [Pg.241]

The results for an equimolar CO -air mixture, obtained with several series of expansions, are presented in Fig.4. The pressure-temperature diagram in the upper part shows the experimental Wilson points and the dew line, which is extrapolated below the triple point For comparison, the frost line is plotted, too. The lower diagram shows the same Wilson points in a plot of the partial density of CO versus temperature. Here, the full curve represents the Wilson line for pure CO, obtained in the preceding investigation [1]. Obviously, spontaneous condensation of CO in the equimolar CO -air mixture begins nearly at the same partial density as with pure CO. ... [Pg.117]

Fig. 5. Phase diagrams of AOT in different solvents and solvent mixtures. Temperature plotted vs. amount of solubilized water. From (24). Fig. 5. Phase diagrams of AOT in different solvents and solvent mixtures. Temperature plotted vs. amount of solubilized water. From (24).
Figure 13.2 Pseudo ternary mixture phase diagram at constant temperature and pressure. The two comers on the base represent a liquid substrate and a gas reactant (having a limited solubility in the substrate) and the top corner corresponds to the solvent. The complete miscibility in (gas + solvent) and (substrate + solvent) ensures the presence of a homogenous region around the solvent corner that can only be obtained for compositions greater than... Figure 13.2 Pseudo ternary mixture phase diagram at constant temperature and pressure. The two comers on the base represent a liquid substrate and a gas reactant (having a limited solubility in the substrate) and the top corner corresponds to the solvent. The complete miscibility in (gas + solvent) and (substrate + solvent) ensures the presence of a homogenous region around the solvent corner that can only be obtained for compositions greater than...
Figure 14.6. Phase diagrams of lyotropic mixtures (temperature versus amphiphile concentration), (a) Hexadecyltrimethylammonium bromide (CTAB)/water, after [50]. L isotropic micellar solution hexagonal phase V bicontinuous cubic phase L lamellar phase C several heterophasic regions containing crystalline components Nc nematic phase of rod-like micelles, (b) Cesium pentadecafluorooctanoate (CsPFO)/water, after [8]. Figure 14.6. Phase diagrams of lyotropic mixtures (temperature versus amphiphile concentration), (a) Hexadecyltrimethylammonium bromide (CTAB)/water, after [50]. L isotropic micellar solution hexagonal phase V bicontinuous cubic phase L lamellar phase C several heterophasic regions containing crystalline components Nc nematic phase of rod-like micelles, (b) Cesium pentadecafluorooctanoate (CsPFO)/water, after [8].
In Fig. 4-9 a constant-temperature diagram for this system has been constructed in which the ordinate is the partial pressure of the components, and the abcissa is the mol fraction of ether in the mixture. This mol fraction is the mols of the ether in the combined liquid phases divided by the total mols of ether and water in all of the liquid present. [Pg.89]

Figure 10. Pressure-temperature diagram for a mixture having a minimum in the bubble point... Figure 10. Pressure-temperature diagram for a mixture having a minimum in the bubble point...
Figure 5.236 Time-temperature diagram of the embrittiement of soft rubber mixtures with a Shore hardness of 50 [795]... Figure 5.236 Time-temperature diagram of the embrittiement of soft rubber mixtures with a Shore hardness of 50 [795]...

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See also in sourсe #XX -- [ Pg.73 ]




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