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Van der Waals equation and

This is the well known equal areas mle derived by Maxwell [3], who enthusiastically publicized van der Waal s equation (see figure A2.3.3. The critical exponents for van der Waals equation are typical mean-field exponents a 0, p = 1/2, y = 1 and 8 = 3. This follows from the assumption, connnon to van der Waals equation and other mean-field theories, that the critical point is an analytic point about which the free energy and other themiodynamic properties can be expanded in a Taylor series. [Pg.445]

Substitution into van der Waals equation and rearrangement leads to only the terms PIP, V/V, and T T, which are called the reduced variables V, and For 1 mole of gas. [Pg.529]

Estimating the critical density IE, ln(Pc7Pc) No consistency test is available for ln(pc7Pc), but for the original Van der Waals equation and the modified VdW equations discussed in this chapter the critical compressibility factors, Zc(VdW) = Pc/(pcRTc), are equal to 3/8 and (a2 - l)/(4a), respectively. In the latter case,... [Pg.421]

A plot of 2 vs. -t2 for symmetrical systems (i.e., ii vo) is shown in Fig. 1 for a series of values of the heat lerm, It shows how the partial vapor pressure of a component of a binary solution deviates positively from Raoult s law more and mure as the components become more unlike in their molecular attractive forces. Second, the place of T in die equation shows that tlic deviation is less die higher the temperature. Third, when the heat term becomes sufficiently large, there are three values of U2 for the same value of ay. This is like the three roots of the van der Waals equation, and corresponds to two liquid phases in equilibrium with each other. The criterion is diat at the critical point the first and second partial differentials of a-i and a are all zero. [Pg.1522]

Table 2.3 A comparison of experimental p versus 1 lv data for 1 mol of C02 at 313 K with values for 1/v generated from the ideal gas law, from a fit to the van der Waals equation, and from the van der Waals equation but using the book values2 for the constants a and b (see text for details)... Table 2.3 A comparison of experimental p versus 1 lv data for 1 mol of C02 at 313 K with values for 1/v generated from the ideal gas law, from a fit to the van der Waals equation, and from the van der Waals equation but using the book values2 for the constants a and b (see text for details)...
The approximate equality of the hi value of the two-dimensional van der Waals equation and the molecular area is not so obvious as might be thought (186a). The b2 value is by definition twice the surface area of a molecule, the diameter of which is d. This diameter is derived from the distance of approach of two colliding molecules. The molecular surface area, however, is derived from the density of liquids, each molecule being assigned its own sphere with a diameter dmm, on the assumption that the molecules are closely packed. As it happens to be that for a great number of molecules... [Pg.82]

THE CONSTANT a FROM THE VAN DER WAALS EQUATION AND THE LATTICE ENERGY CALCULATED ACCORDING TO LONDON... [Pg.346]

If the second partial derivative inside the integral is determined from an EOS, then the heat capacity of a real gas at constant volume can be calculated. For example, the integral in Eq. (1.134) vanishes for the van der Waals equation, and as Eq. (1.129) shows, pressure is a linear function of temperature. However, by using the Berthelot EOS, (Eq. 131), the heat capacity is obtained from Eq. (1.134). [Pg.23]

In this section we introduce several more complex but more accurate equations of state for single species the virial equation, the van der Waals equation, and the Soave-Redlich-Kwong equation. In Section 5.4 we introduce another approach to nonideal gas analysis that makes use of compressibility factors, and we describe Kay s rule, a method for performing PVT calculations on gas mixtures. [Pg.199]

Transforming Van der Waals equation, and arranging in powers of v, we pbtain the equation... [Pg.67]

We begin by calculating the Gibbs free energy of an imperfect gas mixture. Employing the van der Waals equation and inserting the virial coefficient (11.35) into (11.21), remembering that B =B/RT, we have... [Pg.148]

The state equation of an ideal gas is the only one state PV = nRT. They cannot have parameters because they did not depend on the nature of the gas. While the state equation in real gases are the van der Waals equation and the virial coefficients virial equation. They contain parameters because their physical states depend on the nature of the gases. [Pg.213]

Real gases consist of different equation, e.g. van der Waals equation and virial equation. There are parameters that are involved in a real gas which differ according to the different gases used which means that different gases have different parameters. [Pg.213]

The van der Waals Equation and Free Volume Effects More Formal Treatments of Solutions Practical Characterization of Polymers and Solvents Additional Reading... [Pg.643]

Although the discussion of the previous section focused on the van der Waals equation and corresponding-states charts for both the compressibility factor Z and the thermodynamic departure functions, the modem application of the corresponding states idea is to use generalized equations of state. The concept is most easily demonstrated by again using the van der Waals equation of state. From Eqs. 6.2-38,... [Pg.250]

Problem 9.31), where C is a constant whose value depends mon the equation of state used its value is — 1 for the van der Waals equation, and [In (s/2— 1 )]/V2 = —0.623 23 for the Peng-Robinson equation. Combining all of the equations above, we get the following mixing mles ... [Pg.464]

Assume that this associating fluid is described by the van der Waals equation, and in the equation-of-state representation the parameters of the j-mer are gotten from... [Pg.776]


See other pages where Van der Waals equation and is mentioned: [Pg.656]    [Pg.970]    [Pg.817]    [Pg.238]    [Pg.105]    [Pg.263]    [Pg.283]    [Pg.37]    [Pg.1668]    [Pg.1051]    [Pg.150]    [Pg.29]    [Pg.189]    [Pg.210]    [Pg.407]    [Pg.526]    [Pg.136]    [Pg.37]    [Pg.164]    [Pg.474]    [Pg.72]    [Pg.42]    [Pg.651]    [Pg.485]    [Pg.474]   
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