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Vapor pressure data, use

As was described in Chapter 6, the solubility parameter, S, can be used as a diagnostic tool for studying molecular association. Table 12.1 shows some of the relevant data for several aluminum alkyls. The solubility parameters were calculated from vapor pressure data using the procedure described in Chapter 6. [Pg.405]

Na (g). We have calculated the heat of sublimation of sodium to form the monatomic gas from the vapor pressure-temperature data, taking due account of the appreciable amount of Na2 molecules contained in the actual vapor at equilibrium. The vapor pressure data used are those of Edmonson and Egerton,1-2 Rodebush and Walters,1 Rodebush,2 Rodebush and de Vries,1 Rodebush and Henry,1 Haber and Zisch,1 Ladenberg and Minkowski,1 and Gibhart.1 See also Kroner,1 Hackspill,1 van Laar,9 and Simon and Zeidler.1 Our value for the heat of sublimation, Na (c) = Na (g), is —25.9 at 18°. Sherman1 calculated —25.8. [Pg.367]

The solubility parameters of many volatile liquids have been calculated directly from their respective heats of vaporization and molar volumes (Eq. 5). Hoy [32] has shown that 8 for relatively non-volatile liquids can be calculated from vapor pressure data using a modification of the Haggenmacher Eq. [33], Large numbers of such data have been reported and these are collected in extensive tables [27, 28, 34],... [Pg.3]

The vapor pressure data used for evaluation were those corrected by ( ). [Pg.1188]

We particularly welcome estimation methods that incorporate available experimental data, such as melting point. Engineers engage in a number of steps to quantify their confidence in an estimation method and to improve the accuracy of the prediction when working with new molecules. As shown in Table 2, a new molecule with the structure has a molecular weight of 163.606, a measured normal boiling point (T ) of 237.6 C, and a few vapor pressure data. Using an estimation method... [Pg.172]

Expected uncertainty Varies significantly with temperature and with the quality and temperature range of the vapor pressure data used in the correlation. [Pg.515]

Accurate values of the area (S) of the sample used are necessary, since this factor enters into both the expansion equation and into the calculation of the surface free-energy lowering. The method used was that of Brunauer, Emmett, and Teller (7), and the values obtained are given in Table I. Krypton is omitted from the table, since it has been found (5) that the results for this gas are strongly dependent on the particular vapor-pressure data used. [Pg.482]

To examine the effect of the accuracy of the experimental vapor pressure data - used for interpolation and extrapolation purposes - on the quality of the obtained predictions, consider the data for water given below ... [Pg.283]

P the other terms provide corrections which at low or moderate pressure are close to unity. To use Equation (2), we require vapor-pressure data and liquid-density data as a function of temperature. We also require fugacity coefficients, as discussed in Chapter 3. [Pg.40]

Enthalpies are referred to the ideal vapor. The enthalpy of the real vapor is found from zero-pressure heat capacities and from the virial equation of state for non-associated species or, for vapors containing highly dimerized vapors (e.g. organic acids), from the chemical theory of vapor imperfections, as discussed in Chapter 3. For pure components, liquid-phase enthalpies (relative to the ideal vapor) are found from differentiation of the zero-pressure standard-state fugacities these, in turn, are determined from vapor-pressure data, from vapor-phase corrections and liquid-phase densities. If good experimental data are used to determine the standard-state fugacity, the derivative gives enthalpies of liquids to nearly the same precision as that obtained with calorimetric data, and provides reliable heats of vaporization. [Pg.82]

Correlations for standard-state fugacities at 2ero pressure, for the temperature range 200° to 600°K, were generated for pure fluids using the best available vapor-pressure data. [Pg.138]

Polymer simulations can be mapped onto the Flory-Huggins lattice model. For this purpose, DPD can be considered an off-lattice version of the Flory-Huggins simulation. It uses a Flory-Huggins x (chi) parameter. The best way to obtain % is from vapor pressure data. Molecular modeling can be used to determine x, but it is less reliable. In order to run a simulation, a bead size for each bead type and a x parameter for each pair of beads must be known. [Pg.274]

Ref. 87. Test method ASTM E96-35T (at vapor pressure for 25.4 p.m film thickness). Values are averages only and not for specification purposes. Original data converted to SI units using vapor pressure data from Ref. 90. [Pg.352]

Original data converted to SI units using vapor pressure data from Ref. 72. "At20°C. [Pg.361]

Corresponding states have been used in other equations. For example, the Peng-Robinson equation is a modified RedHch-Kwong equation formulated to better correlate vapor—Hquid equiHbrium (VLE) vapor pressure data. This equation, however, is not useful in reduced form because it is specifically designed to calculate accurate pressure data. Reduced equations generally presuppose knowledge of the pressure. [Pg.240]

Values of the compound speciBc constants m and c were originally derived by Othmer et al. and greatly expanded to over 600 common organics by Danner and Daiibert. If constants are not available but any two vapor pressure data points are available, the constants m and C can be calculated using Eqs. (2-46) and (2-47). [Pg.391]

Pure-component vapor pressures can be used for predicting solu-bihties for systems in which RaoiilFs law is valid. For such systems Pa = Pa a, where p° is the pure-component vapor pressure of the solute andp is its partial pressure. Extreme care should be exercised when attempting to use pure-component vapor pressures to predict gas-absorption behavior. Both liquid-phase and vapor-phase nonidealities can cause significant deviations from the behavior predicted from pure-component vapor pressures in combination with Raoult s law. Vapor-pressure data are available in Sec. 3 for a variety of materials. [Pg.1351]

Determine the vent size for a vapor pressure system using the following data and physical properties. [Pg.1000]

Using the vapor pressure data for benzene and toluene [59] ... [Pg.26]

It is desired to separate a non-volatile material from an equimolal mixture of benzene, toluene, and xylene at 80°C. Vapor pressure data for these compounds are shown in several physical property sources. The following approximate values for the specific heats and latent heats of vaporization may be used ... [Pg.61]

This suggests that a plot of P against 1/T should yield a line having a local slope of (-A, /R). A straight line is obtained only when is nearly constant, i.e., over a narrow range of temperatures. An integrated version of the Clausius-Clapeyron equation finds use in correlation of vapor pressure data ... [Pg.346]

Two estimates will be made using vapor pressure data from the CRC Handbook [63] and the integrated form of Clausius-Clapeyron equation ... [Pg.347]

The advantages of vapor pressure as an index of moisture have been discussed. At the present time very few vapor pressure data are available for foods. It would be of great interest to measure vapor pressure concurrently with the moisture content in order to determine the usefulness of the vapor pressure in studies on the stability of dehydrated foods. [Pg.53]

E8,6 Use the following vapor pressure data for solid palladium metal as a function of temperature,7 to calculate ASUb//m. the mean enthalpy of sublimation of palladium. [Pg.428]

Thus, if the saturated vapor pressure is known at the azeotropic composition, the activity coefficient can be calculated. If the composition of the azeotrope is known, then the compositions and activity of the coefficients at the azeotrope can be substituted into the Wilson equation to determine the interaction parameters. For the 2-propanol-water system, the azeotropic composition of 2-propanol can be assumed to be at a mole fraction of 0.69 and temperature of 353.4 K at 1 atm. By combining Equation 4.93 with the Wilson equation for a binary system, set up two simultaneous equations and solve Au and A21. Vapor pressure data can be taken from Table 4.11 and the universal gas constant can be taken to be 8.3145 kJ-kmol 1-K 1. Then, using the values of molar volume in Table 4.12, calculate the interaction parameters for the Wilson equation and compare with the values in Table 4.12. [Pg.75]

A distillation column uses a partial condenser as shown in Figure 9.19. Assume that the reflux ratio and the overhead product composition and flowrate and the operating pressure are known and that the behavior of the liquid and vapor phases in the column is ideal (i.e. Raoult s Law holds). How can the flowrate and composition of the vapor feed to the condenser and its liquid products be estimated, given the vapor pressure data for the pure components. Set up the equations that need to be solved. [Pg.179]

Availability of Physical Properties Data and Model Parameters. We have found that the development of a data base for physical properties and other model parameters is as time consuming, and intellectually demanding, as the development of the model itself. One will be surprised to know, for example, that vapor pressure data at around 25°C for many commonly used solvents are non-existent. [Pg.177]

This can be empirically modified by introducing additional parameters to give the three-parameter Antoine equation by replacing T with (T + C), where C is a constant, which is the most common vapor pressure correlation used to represent experimental data (Zwolinski and Wilhoit 1971, Boublik et al. 1984, Stephenson and Malanowski 1987, and other handbooks). [Pg.6]

The optimum data are selected in step l by using a precalculated standard deviation, which is directly related to the constancy of temperature. These selected sets of data are used in step 2 for calculation of equilibrium vapor pressures by means of the Knudsen equation. A regression analysis of these vapor pressure data is then carried out in step 3. [Pg.138]

To prove that this method can be applied also to solids with strong ionic bonding, NaCl was investigated as an example. Also in this case an aluminia Knudsen cell was used, the orifice diameter was calibrated with gold. Figure 69 shows a graphical presentation of the vapor pressure data obtained, compared with data from the literature (Kelly)68. ... [Pg.140]


See other pages where Vapor pressure data, use is mentioned: [Pg.609]    [Pg.520]    [Pg.1625]    [Pg.56]    [Pg.438]    [Pg.176]    [Pg.609]    [Pg.520]    [Pg.1625]    [Pg.56]    [Pg.438]    [Pg.176]    [Pg.464]    [Pg.1259]    [Pg.305]    [Pg.378]    [Pg.213]    [Pg.60]    [Pg.178]    [Pg.115]    [Pg.136]    [Pg.471]    [Pg.87]    [Pg.352]   
See also in sourсe #XX -- [ Pg.534 ]




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