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Ethanol temperature-composition

Deviations from Raoult s law can make it impossible to separate liquids by distillation. The temperature-composition diagrams for mixtures of ethanol and benzene and of acetone and chloroform show why. A positive deviation from Raoult s law means that the attractive forces between solute and solvent are lower than those between the molecules of the pure components. As a result, the boiling point of the mixture is lower than that predicted by Raoult s law. For some pairs of components, the boiling point of the mixture is in fact lower than the boiling point of either constituent (Fig. 8.41). A mixture for which the lowest boiling temperature is below... [Pg.462]

FIGURE 8.41 The temperature composition diagram of a minimum-boiling azeotrope (such as ethanol and benzene). When this mixture is fractionally distilled, the (more volatile) azeotropic mixture is obtained as the initial distillate. [Pg.462]

Figure 1 shows the equilibrium data for the ethanol-water systems saturated with copper(II) chloride, strontium chloride, or nickel(II) chloride. Figure 2 shows the temperature-compositions diagrams corrected to 700 mmHg. [Pg.93]

The data in Tables I-XVI (see Appendix for all tables) show the isobaric vapor-liquid equilibrium results at the boiling point for potassium, ammonium, tetramethylammonium, tetraethylammonium, tetra-n-propylammonium, and tetra-n-butylammonium bromides in various ethanol-water mixtures at fixed liquid composition ratios. The temperature, t, is the boiling temperature for all solutions in these tables. In all cases, the ethanol-water composition was held constant between 0.20 and 0.35 mole fraction ethanol since it is in this range that the most dramatic salt effects on vapor-liquid equilibrium in this particular system should be observed. That is, previous data (12-15,38) have demonstrated that a maximum displacement of the vapor-liquid equilibrium curve by salts frequently occurs in this region. In the results presented here, it should be noted that Equation 1 has been modified to... [Pg.109]

Changing the recovery of ethanol from 99-99.99%m produces only minor increases in the heat loads. A summary of the column material balance for one mole of feed is shown in Table V when the solvent-feed ratio is 3.5 mole basis. This calculation was made for a recovery of 99.99% ra ethanol using 46 equilibrium trays with the solvent on 43 and the feed on 22. The reflux-feed ratio was 1.5537 mole basis. The corresponding data for temperature, composition, and volatility profiles are summarized in Table VI. [Pg.16]

Figure 3.5 Phase diagram for mixtures of n-heptane and ethanol, which exhibits a low boiling azeotrope (a) temperature-composition diagram at 30.1°C, and (b) pressure-composition diagram at 1 atm. Data taken from JD Raal, RK Code, and DA Best, J. Chem. Eng. Data 17, 211 (1972). Figure 3.5 Phase diagram for mixtures of n-heptane and ethanol, which exhibits a low boiling azeotrope (a) temperature-composition diagram at 30.1°C, and (b) pressure-composition diagram at 1 atm. Data taken from JD Raal, RK Code, and DA Best, J. Chem. Eng. Data 17, 211 (1972).
Mixtures o( benzene (b.pt. 80 °C) and ethanol show a native deviation from Raoult s Law. Give a filJly labelled temperature-composition diagram for such mixtures and state and explain what happens vdtm benzene is added to ethanol. [Pg.138]

Figure 6.11 shows a pressure-composition liquid-vapor phase diagram of ethanol and diethyl ether for a fixed temperature of 20 C. Compare Figure 6.11 with Figure 6.2, which represents the nearly ideal mixmre of benzene and toluene. Figure 6.12 shows the temperature-composition phase diagram of the same mixture for a fixed pressure of 1.84 atm. Compare this figure with Figure 6.3. This system exhibits positive deviation from Raoult s law. The vapor pressure is larger than it would be if the solution were ideal, and the solution boils at a lower temperature than if it were an ideal solution. Figure 6.11 shows a pressure-composition liquid-vapor phase diagram of ethanol and diethyl ether for a fixed temperature of 20 C. Compare Figure 6.11 with Figure 6.2, which represents the nearly ideal mixmre of benzene and toluene. Figure 6.12 shows the temperature-composition phase diagram of the same mixture for a fixed pressure of 1.84 atm. Compare this figure with Figure 6.3. This system exhibits positive deviation from Raoult s law. The vapor pressure is larger than it would be if the solution were ideal, and the solution boils at a lower temperature than if it were an ideal solution.
Figure 6.12 Temperature-Composition Phase Diagram for Diethyl Ether-Ethanol at 1.84 atm. The lower curve represents the temperature as a function of mole fraction in the liquid, and the upper curve represents the temperature as a function of mole fraction in the vapor. Drawn from data in J. Timmermans, Physicochemical Constants of Binary Systems, Vol. 2, Interscience Publishers, New York, 1959, p. 401. Figure 6.12 Temperature-Composition Phase Diagram for Diethyl Ether-Ethanol at 1.84 atm. The lower curve represents the temperature as a function of mole fraction in the liquid, and the upper curve represents the temperature as a function of mole fraction in the vapor. Drawn from data in J. Timmermans, Physicochemical Constants of Binary Systems, Vol. 2, Interscience Publishers, New York, 1959, p. 401.
FIGURE 8.17 Temperature-composition diagram for ethanol-water at 1 atm, using data points from [1]. The curves are simple smooth interpolations. The arrows show the graphical solution for the bubble point (temperature-specified) and vapor composition. [Pg.128]

Submerged culture oxidizers can also be operated on a continuous basis. Continuous monitoring of ethanol and acetic acid concentrations, temperature, and aeration rates permit control of feed and withdrawal streams. Optimum production, however, is achieved by semicontinuous operation because the composition of vinegar desired in the withdrawal stream is so low in ethanol that vigorous bacterial growth is impeded. Bacterial... [Pg.409]

The numerical constants were obtained over the temperature range of 5°C to 45°C and a concentration range of 0 to 0.5 volume fraction of ethanol inn-hexane.The effect of temperature and solvent composition on solute retention can, again, be best displayed by the use of 3-D graphs, and curves relating both temperature and solvent composition to the retention volume of the (S) enantiomer of 4-benzyl-2-oxazolidinone are shown in Figure 23. Figure 23 shows that the volume fraction of ethanol in the solvent mixture has the major impact on solute retention. [Pg.120]

The effect of temperature, although significant, is not nearly as great as that from the ethanol content and is greatest at low concentrations of the polar solvent. It is clear, that the solute retention is the least at high ethanol concentrations and high temperatures, which would provide shorter analysis times providing the selectivity of the phase system was not impaired. The combined effect of temperature and solvent composition on selectivity, however, is more complicated and to some extent... [Pg.120]

Scott and Beesley [2] measured the corrected retention volumes of the enantiomers of 4-benzyl-2-oxazolidinone employing hexane/ethanol mixtures as the mobile phase and correlated the corrected retention volume of each isomer to the reciprocal of the volume fraction of ethanol. The results they obtained at 25°C are shown in Figure 8. It is seen that the correlation is excellent and was equally so for four other temperatures that were examined. From the same experiments carried out at different absolute temperatures (T) and at different volume fractions of ethanol (c), the effect of temperature and mobile composition was identified using the equation for the free energy of distribution and the reciprocal relationship between the solvent composition and retention. [Pg.158]

Sample Preparation. Liquid crystalline phases, i.e. cubic and lamellar phases, were prepared by weighing the components in stoppered test tubes or into glass ampoules (which were flame-sealed). Water soluble substances were added to the system as water solutions. The hydrophobic substances were dissolved in ethanol together with MO, and the ethanol was then removed under reduced pressure. The mixing of water and MO solutions were made at about 40 C, by adding the MO solution dropwise. The samples for the in vivo study were made under aseptic conditions. The tubes and ampoules were allowed to equilibrate for typically five days in the dark at room temperature. The phases formed were examined by visual inspection using crossed polarizers. The compositions for all the samples used in this work are given in Tables II and III. [Pg.252]


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