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Molar density functional dependence

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]

Gases Gases/vapors are compressible and their densities are strong functions of both temperature and pressure. Equations of state (EoS) are commonly used to correlate molar densities or molar volumes. The most accurate EoS are those developed for specific fluids with parameters regressed from all available data for that fluid. Super EoS are available (or some of the most industrially important gases and may contain 50 or more constants specific to that chemical. Different predictive methods may be used for gas densities depending upon the conditions ... [Pg.526]

When taking these partial derivatives it must be remembered that, in general, the molar densities, the mass transfer coefficients, and thermodynamic properties are functions of temperature, pressure, and composition. In addition, H is a function of the molar fluxes. We have ignored most of these dependencies in deriving the expressions given above. The important exception is the dependence of the K values on temperature and composition that cannot be ignored. The derivatives of the K values with respect to the vapor mole fractions are zero in this case since the model used to evaluate the K values is independent of the vapor composition. [Pg.288]

A simple graph theoretical distinction was made between "extensive" (molar) properties which depend on the amount of material present and "intensive" properties which do not. (The molecular weight per repeat imit, the molar volume, and the molar glass transition function, are examples of extensive properties. The density and the glass transition temperature are examples of intensive properties.)... [Pg.47]

Two different reactions occur together in solution. One of them is quenched by oxygen and by cyclooctatetraene, and becomes the only significant process when a sensitiser is used. Its products are both syn and anti dimers, in a ratio dependent on solvent og(antilsyn) is a linear function of [(e— l)/(2e-f-1 )]p (where p is the molar density of solvent), with a negative slope . The rate of this reaction is particularly high in heavy-atom solvents, like /i-PrBr, Mel and EtI. that are known to catalyse intersystem crossing and increase the concentration of triplet states in one case yields are directly related to the square of the spin-orbit coupling factor of bromine and iodine atoms. ... [Pg.151]

Hence, 0a = 1, by definition. In summary, aU partial pressures in the rate law should be written as a product of total pressure and mole fraction. Then, mole fractions can be expressed in terms of the conversion of CO. Alternatively, the ideal gas law can be used to express partial pressures p, as QRT, and the conversion dependence of molar density C, is tabulated by Fogler (1999, p. 96) for variable-volume gas-phase flow reactors. It should be emphasized that y, ptotai and CiRT generate the same function of conversion when the s parameter in Fogler s expressions is written as... [Pg.59]

FUNCTIONAL DEPENDENCE OE THE MOLAR DENSITY OF SPECIES i VIA DIMENSIONAL ANALYSIS... [Pg.269]

The physical meaning of the function p k) is the density of probability of the stability constant k and is connected with experimental data, i.e. the change in the concentration of metal ions in solution and unreacted functional groups, or the concentration of surface sites occupied by metal ionsy([M]). At p( ) > 0 the equilibrium constant can be presented as an average equilibrium function depending on the molar concentration, Cj, of the real species M,P (/ = 1,. .. s) and on the fraction of occupied sites in a macromolecule, 0. [Pg.75]

Here the p,- are pure component molar densities and the AA.,y are parameters that depend on the identities of species i and The AX,y are often assumed to be independent of state condition alternatively, they may be modeled as simple functions of T. But usually (5.6.30) allows the two temperature-dependent parameters A 2 - 21... [Pg.218]

In the thermodynamics of critical phenomena one prefers alternative thermodynamic variables and alternative variable-dependent thermodynamic potentials, namely, the density of the Helmholtz energy A/V as a function of temperature and molar density p = n/V, or the pressure P as a function of temperature and chemical potential p = G/n = d A/V)/dp r [1, 2]. The corresponding differential equations for the density-dependent potential A/V and for the field-dependent potential P read... [Pg.90]

Values of domain size and separation were discussed in terms of Helfand s NIA theory, tacitly assuming that the two components of the block copolymer constituted a symmetric polymer pair, i.e. equality of Kuhn statistical step lengths, b, and monomer molar density. Whilst this is approximately true for values of b for styrene and isoprene, the densities are quite different. However, calculations of domain size and domain separation as a function of molecular weight for both styrene and isoprene domains show that both types have the same molecular weight dependence and moreover the difference in the values for either styrene or isoprene domains is negligible. Figure 10... [Pg.19]

Molality is used in thermodynamic calculations where a temperature independent unit of concentration is needed. Molarity, formality and normality are based on the volume of solution in which the solute is dissolved. Since density is a temperature dependent property a solution s volume, and thus its molar, formal and normal concentrations, will change as a function of its temperature. By using the solvent s mass in place of its volume, the resulting concentration becomes independent of temperature. [Pg.18]

In a variable-density reactor the residence time depends on the conversion (and on the selectivity in a multiple-reaction system). Also, in ary reactor involving gases, the density is also a function of reactor pressure and temperature, even if there is no change in number of moles in the reaction. Therefore, we frequently base reactor performance on the number of moles or mass of reactants processed per unit time, based on the molar or mass flow rates of the feed into the reactor. These feed variables can be kept constant as reactor parameters such as conversion, T, and P are varied. [Pg.107]

Instruments with indirect pressure measurement. In this case, the pressure is determined as a function of a pressure-dependent (or more accurately, density-dependent) property (thermal conductivity, ionization probability, electrical conductivity) of the gas. These properties are dependent on the molar mass as well as on the pressure. The pressure reading of the measuring instrument depends on the type of gas. [Pg.76]

Recently, Rebelo and coworkers [172] presented a method to estimate the critical temperatures of some ILs based on fhe temperature dependence of fheir surface tension and liquid densities. The molar enfhalpies of vaporization of a series of commonly used ILs were also determined for fhe firsf fime. The molar enfhalpies of vaporization of [C Cilm][Tf2N] ILs in fhe function of the alkyl chain length have been presented [214]. The critical properties (T(, P(, Vf), the normal boiling temperatures, and the acentric factors of 50 ILs were determined as well for fhe firsf fime [215]. [Pg.59]


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See also in sourсe #XX -- [ Pg.269 , Pg.270 ]




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