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Reduced vapor pressures

For these reasons, ethanol is most likely to find use as a motor fuel in the form of a gasoline additive, either as ethanol or ethanol-based ethers. In these blend uses, ethanol can capture the high market value of gasoline components that provide high octane and reduced vapor pressure. [Pg.423]

Halogenated All l Phosphates and Phosphonates. In this important class of additives, the halogen contributes somewhat to flame retardancy although this contribution is offset by the lower phosphoms content. The halogens reduce vapor pressure and water solubHity, thus aiding retention of these additives. Efficient manufacturing processes lead to favorable economics. [Pg.476]

The accurate representation of vapor pressure data over a wide temperature range requires an equation of greater complexity. The Wagner equation (eq. 22) expresses the reduced vapor pressure as a function of reduced temperature TIT/... [Pg.484]

Three Parameter Models. Most fluids deviate from the predicted corresponding states values. Thus the acentric factor, CO, was introduced to account for asymmetry in molecular stmcture (79). The acentric factor is defined as the deviation of reduced vapor pressure from 0.1, measured at a reduced temperature of 0.7. In equation form this becomes ... [Pg.240]

Acentric Factor The acentric facdor of a compound (co) is primarily a measure of the shape of a molecule, though it also measures a molecules polarity. It is calculated from the reduced vapor pressure (P ) at a reduced temperature of 0.7 by the definition, Eq. (2-23). [Pg.389]

Vapour-pressure-dependent up to svp, supplying the same data as in (1) per test tests likely to be medium-term to give sufficient permeant for reliable measurement. Can reduce vapor pressure (e.g., by using a carrier gas) on low-pressure side to maximize permeation by keeping P2 near-zero. [Pg.645]

Essentially pressure-independent only permeation rate and D readily obtainable medium-long tests (again can be shortened by reducing vapor pressure on low pressure side). [Pg.646]

Fig. 1. Mean reduced vapor pressure curve for the halides of sodium, potassium, rubidium, and cesium. Average deviation from the mean is shown by the vertical lines. Fig. 1. Mean reduced vapor pressure curve for the halides of sodium, potassium, rubidium, and cesium. Average deviation from the mean is shown by the vertical lines.
Fig. 13.1 Reduced vapor pressure and molar density vs. reciprocal reduced temperature for HoO, CH4, H2, and 4He. In each case, were simple corresponding states theory adequate, all data would lie on a single master curve. Using extended CS the curves are fit to acceptable precision, (a) (top) = reduced vapor pressures, (b) (bottom) = reduced liquid molar densities... [Pg.415]

Figure 13.1a shows reduced vapor pressures and Fig. 13.1b reduced liquid molar densities for the parent isotopomers of the reference compounds. Such data can be fit to acceptable precision with an extended four parameter CS model, for example using a modified Van der Waals equation. In each case the parameters are defined in terms of the three critical properties plus one system specific parameter (e.g. Pitzer acentric factor). Were simple corresponding states theory adequate, the data for all... [Pg.415]

Solutions in hand for the reference pairs, it is useful to write out empirical smoothing expressions for the rectilinear densities, reduced density differences, and reduced vapor pressures as functions of Tr and a, following which prediction of reduced liquid densities and vapor pressures is straightforward for systems where Tex and a (equivalently co) are known. If, in addition, the critical property IE s, ln(Tc /Tc), ln(PcVPc), and ln(pcVPc), are available from experiment, theory, or empirical correlation, one can calculate the molar density and vapor pressure IE s for 0.5 < Tr < 1, provided, for VPIE, that Aa/a is known or can be estimated. Thus to calculate liquid density IE s one uses the observed IE on Tc, ln(Tc /Tc), to find (Tr /Tr) at any temperature of interest, and employs the smoothing relations (or numerically solves Equation 13.1) to obtain (pR /pR). Since (MpIE)R = ln(pR /pR) = ln[(p /pc )/(p/pc)] it follows that ln(p7p)(MpIE)R- -ln(pcVpc). For VPIE s one proceeds similarly, substituting reduced temperatures, critical pressures and Aa/a into the smoothing equations to find ln(P /P)RED and thence ln(P /P), since ln(P /P) = I n( Pr /Pr) + In (Pc /Pc)- The approach outlined for molar density IE cannot be used to rationalize the vapor pressure IE without the introduction of isotope dependent system parameters Aa/a. [Pg.419]

Stabilizer a fractionating tower for removing light hydrocarbons from an oil to reduce vapor pressure particularly applied to gasoline. [Pg.454]

A pure component constant that is occasionally used in property correlations is the enthalpy of vaporization at the normal boiling point, AHvbp. In addition, several special estimation methods are suggested. The Chen equation (15) gives a relation among the enthalpy of vaporization, the reduced vapor pressure, and the reduced temperature. When applied to the normal boiling point, Eq. 2 is obtained, with an average error of 2% ... [Pg.695]

For a given relative humidity (RH) and temperature, values are assumed for two of the three variables, t, D0 and Du and the third is calculated. In this way, droplets of various initial diameter can be calculated to evaporate to any assumed diameter Dt after t seconds of fall at terminal velocity. The equation corrects for the effect of fall velocity on evaporation rate and the concurrent effect of changing diameter on fall velocity. It assumes constant air temperature and pressure, a large volume of air per droplet so that the air humidity is relatively unaffected, no air turbulence, and the absence of solutes which reduce vapor pressure or form evaporation-retarding films at the surface of the droplet. It further assumes terminal fall velocity at all times. With these restrictions, the theory appears valid for droplet sizes that obey Stokes s law. [Pg.150]

Figure 3.11 Approximate temperature dependence of reduced vapor pressure. Figure 3.11 Approximate temperature dependence of reduced vapor pressure.
The observation that the properties could be expressed in terms of the reduced quantities had many important ramifications. These including the possibility that if you plotted the reduced vapor pressure as a function of reduced temperature, all substances would fall onto a single curve. Furthermore, if you plotted the compressibility factor versus the reduced pressure with the reduced temperature as a parameter, all fluids would lie on the same plot. [Pg.39]

The results stated so far has been with saturated vapor or liquid as the equilibrium bulk phase. Liquid-like state in pore, however, can hold with reduced vapor pressure in bulk the well-known capillary condensed state. One of the most important feature of the capillary condensation is the liquid s pressure Young-Laplace effect of the curved surface of the capillary-condensed liquid will pull up the liquid and reduce its pressure, which can easily reach down to a negative value. In the section 2 we modeled the elevated freezing point as a result of increased pressure caused by the compression by the excess potential. An extension of this concept will lead to an expectation that the capillary-condensed liquid, or liquid under tensile condition, must be accompanied with depressed freezing temperature compared with that under saturated vapor. Then, even at a constant temperature, a reduction in equilibrium vapor pressure would cause phase transition. In the following another simulation study will show this behavior. [Pg.36]

Again the graphical representation used by the interactive design enables us to evaluate the effect of any substitution. Replacing, —Cl by 0=CH—, would result in a compound having reduced vapor pressure, an increased enthalpy of vaporization, and an increased liquid heat capacity. These alterations of physical properties are derived from the relative positions of the group vectors and the locations of the constraints. [Pg.299]


See other pages where Reduced vapor pressures is mentioned: [Pg.527]    [Pg.496]    [Pg.278]    [Pg.7]    [Pg.918]    [Pg.496]    [Pg.141]    [Pg.567]    [Pg.278]    [Pg.107]    [Pg.34]    [Pg.155]    [Pg.39]    [Pg.40]    [Pg.51]    [Pg.28]    [Pg.278]    [Pg.527]    [Pg.50]    [Pg.91]    [Pg.384]    [Pg.275]    [Pg.405]    [Pg.493]   
See also in sourсe #XX -- [ Pg.415 , Pg.419 ]




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