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Residual Helmholtz energy

The second term on the right-hand side of Equation (1) is the residual Helmholtz energy of mixing for an Ising mixture (AmixFrIsing). Its expression will be discussed below. [Pg.161]

Residual Helmholtz energy of mixing for multicomponent Ising mixture... [Pg.163]

Equation (12) can be used to calculate the residual Helmholtz energy of mixing (AmixFrIsing) of monomer mixture of polymer system in step 2 of Figure 1. However, the mole fraction x, should be replaced by volume fraction ,. We have... [Pg.166]

The residual Helmholtz energy of dissociation and association of polymer chains... [Pg.166]

The residual Helmholtz energy due to the dissociation of polymer chains in pure state and the association of polymer chains in mixture state can be calculate by Equation (5). The pair correlation functions of component i in the corresponding Ising lattice system are calculated by gf = 1 / fyfij (Liu al., 2007). The residual... [Pg.166]

Zcoii/y is the sum of two Gaussians, the first centered at y = 0 to ensure the correct behavior in the limit of zero density, and the second centered at the rectilinear diameter yT to provide the correct value of residual Helmholtz energy at high density. The temperature dependence of yu is given universal [2], The parameters b and c, which determine the second and third virial coefficients, are given universally for non-polar substances [3]. The pre-exponential factor w has a dominating influence on the vapor pressure. Its temperature dependence requires two substance-specific correction parameters wi and w2. [Pg.406]

It is also possible to calculate mixture phase equilibria based on the reference-quality equations of state described in Section 1.2.4. In this approach, the Helmholtz energy is written as the sum of pure-component contributions (given by the reference-quality EOS for each pure component) plus a residual term. The residual term contains one or more adjustable parameters for each binary. Software implementing this approach is available [9]. [Pg.12]

The statistical-associated fluid theory (SAFT) of Chapman et al. [25, 26] is based on the perturbation theory of Wertheim [27]. The model molecule is a chain of hard spheres that is perturbed with a dispersion attractive potential and association potential. The residual Helmholtz energy of the fluid is given by the sum of the Helmholtz energies of the initially free hard spheres bonding the hard spheres to form a chain the dispersion attractive potential and the association potential,... [Pg.308]

To obtain internal energy from an eos, we first obtain its residual function by combining the residual Helmholtz energy and residual entropy,... [Pg.319]

In addition to the above direct tests, the rule given by Equation 6 was tested by calculating the thermodynamic excess functions of mixtures. The relations are given by Kreglewski and Chen (8). The basic one for the residual Helmholtz energy of a mixture Amr is... [Pg.206]

The isometric residual chemical potential can be obtained from that part of (3.2.22) which relates the chemical potential to the Helmholtz energy. [Pg.136]

With m , and s" determined, we can use the defining Legendre transforms to relate the residual Gibbs energy, Helmholtz energy, and chemical potential. The results are... [Pg.137]

An alternative and very successful approach, which was pursued particularly over the last two decades, is the appHcation of perturbation theories. The main assumption here is that the residual (difference from the ideal-gas state) part of the Helmholtz energy of a system (and hence also the system pressure) can be written as sum of different terms. The main contribution is described by the Helmholtz energy of a chosen reference system Contributions to the Hehnholtz energy which are not covered by the reference system are considered as perturbations and are described by AP . [Pg.28]

The simplest fundamental connection between equations of state, expressed as Helmholtz functions of T, v, and x, and correlation function integrals is via the second composition derivative of the residual Helmholtz energy and DCFI,... [Pg.252]

Like reference equations, state-of-the-art technical EOS are formulated in terms of the Helmholtz energy, which is split into an ideal gas part and a residual part. Instead of the specific volume, the density is used as a variable ... [Pg.34]

The more difficult part is to set up a correlation for the residual part of the Helmholtz energy a (r, 5). For this purpose, a bank of terms that could be useful for a high-precision equation of state has been established (29]. The general setup for the fitting procedure contains 583 terms. It is expressed as... [Pg.35]

According to the relationship between excess property and residual part of the Helmholtz energy... [Pg.167]

Ehe residual Helmholtz energy consists of the hard-chain reference, and the dispersion contribution, Additionally, contributions arising from polir interaction, and association, can be included. The overall Helmholtz energy reads... [Pg.464]

Anderko and Pitzer (1991, 1993a,b), Jiang and Pitzer (1996), Pitzer (1998), and Anderko et al. (2002) developed an EOS for geologically and industrially important aqueous electrolyte solutions H2O + NaCl, H2O + KCl, and H2O + CaCl2. These equations are based on a theoretical model for mixtures of hard spheres with appropriate diameters and dipole moments for H2O, NaCl, and KCl and with a quad-rupole moment for CaCl2. Residual Helmholtz energy have been defined as (Pitzer, 1998)... [Pg.147]

The Helmholtz energy is convenient as a generating thermodynamic function because its derivatives, with respect to volmne and each of the components moles numbers, yield the pressme and the chemical potentials, respectively. The residual Helmholtz energy is then... [Pg.147]

The shape factors are weak functions of temperature and, in principle, density and can be visualized as distorting scales that force the two fluids to conformality. Although there is no direct theoretical evidence for the density dependence of the shape factors, mathematical solutions for exact shape factors found by equating the dimensionless residual compressibility factor and Helmholtz energy of two pure-fluids exhibit weak density dependence. [Pg.142]

The parameters Qa and are universal for this equation of state and m (o) is a simple quadratic function of the acentric factor. The residual compressibility factor and dimensionless residual Helmholtz energy are given by... [Pg.155]

The approach of Kiselev, based on the work of Sengers and co-workers and Kiselev and co-workers, " utilizes a renormalized Landau expansion that smoothly transforms the classical Helmholtz energy density into an equation that incorporates the fluctuation-induced singular scaling laws near the critical point, and reduces to the classical expression far from the critical point. The Helmholtz energy density is separated into ideal and residual terms, and the crossover function applied to the critical part of the Helmholtz energy Aa(AT, Av), where Aa(AT, Av) = a(T, v) — a, g(T, v) and the background contribution abg(T, v) is expressed as. [Pg.231]

In eqs 8.39 and 8.40 AT=TITqc— 1 and Av = v/vqc— 1 are dimensionless distances from the calculated classical critical temperature (Toc) and classical critical molar volume (vqc), ao(T) is the dimensionless temperature-dependent ideal-gas term, and Po(T) = P T,vo c)vo,c/RT and a T,v) are the dimensionless pressure and residual Helmholtz energy along the critical isochore, respectively. The AT and Av are then replaced with the renormalized values in... [Pg.231]

In a similar way, data can be non-linear if they are measured, for example, as a function of temperature and pressure instead of temperature and density or if their relation to the reduced Helmholtz energy results in residual that eontains nonlinear combinations of the derivatives of oZ. In the first case, the density p(expt) has to be replaced by a density pjcalc, J(expt), />(expt), n, which has to be continuously updated throughout the fitting process. This is the case for example for enthalpy... [Pg.400]

In 1940, Benedict, Webb, and Rubin published their formulation both in terms of pressure and in the residual Helmholtz energy. However, the formulation in pressure was considered the original formulation, and the Helmholtz energy formulation was rarely used because the ideal gas contribution was missing. The first equation of state that was formulated exclusively in terms of the Helmholtz energy a was published in 1969 by Keenan et al for water and steam. The equation is given in specific quantities by... [Pg.409]

The empirical function Q p, r) of eq 12.30 describes the residual contribution to the Helmholtz energy and is expressed as... [Pg.409]

Today, this equation of state has fifty adjustable parameters. Ay, to represent the residual of the Helmholtz energy and in this respect is interesting only from a historical perspective. [Pg.409]

In this equation, C is the number of components in the mixture, A i is the ideal gas Helmholtz energy for component i, and is the pure fluid residual Helmholtz energy of component i evaluated at a reduced density and temperature defined below. [Pg.426]

The thermodynamic properties required to calculate phase equilibria are obtained by dilferentiating the residual Helmholtz energy. The association contributions to the compressibility factor Z and the fugacity coefficient of component i in the mixture are given by ... [Pg.444]


See other pages where Residual Helmholtz energy is mentioned: [Pg.153]    [Pg.153]    [Pg.158]    [Pg.160]    [Pg.160]    [Pg.161]    [Pg.317]    [Pg.136]    [Pg.167]    [Pg.385]    [Pg.771]    [Pg.668]    [Pg.119]    [Pg.223]    [Pg.399]    [Pg.399]    [Pg.399]    [Pg.400]    [Pg.440]   


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