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Equation auxiliary

In addition to the continuity equations and the expressions for rate coefficients and equilibrium constants, several further relationships are required in order to close the system of equations. Apart from the expressions for the transport fluxes, these are [Pg.29]

The continuity equations of Sections 2.1 to 2.4 have been derived for a reference frame which is stationary in space. This is known as an Eulerian frame of reference, and in it at the steady state the time derivatives vanish, as in [Pg.29]

and (2.21). This reference frame is particularly useful for examination of the properties of steady-state reaction systems such as flames on burners, which are themselves stationary in space. The convection terms remain in the equations. [Pg.30]

The convection terms have now disappeared from the equations. [Pg.30]

After finalizing the governing equations, it is necessary to provide auxiliary equations to estimate fluid properties and to specify appropriate initial and boundary conditions. These aspects are discussed in the next section. [Pg.44]

To close the set of model equations, it is necessary to specify equations to prescribe or describe fluid density and other fluid properties such as viscosity, diffusivity, thermal conductivity and heat capacity. It is possible to treat these properties either as constants or as functions of thermodynamic variables and/or compositions. For example, the dependence of fluid density on composition, temperature and pressure can be described by the following equation  [Pg.44]

For ideal gases, it is possible to write component density, Pk in terms of the molecular weight of component k, temperature, operating pressure and universal gas constant. For non-ideal fluids, one can use empirical correlations to represent [Pg.44]


In principle, given expressions for the crystallization kinetics and solubility of the system, equation 9.1 can be solved (along with its auxiliary equations -Chapter 3) to predict the performance of continuous crystallizers, at either steady- or unsteady-state (Chapter 7). As is evident, however, the general population balance equations are complex and thus numerical methods are required for their general solution. Nevertheless, some useful analytic solutions for design purposes are available for particular cases. [Pg.264]

V. The auxiliary equation is normally an algebraic equation rather than an ODE. In chemical engineering problems, it will usually be an equation of state, such as the ideal gas law. In any case, the set of ODEs can be integrated numerically starting with known initial conditions, and V can be calculated and updated as necessary. Using Euler s method, V is determined at each time step... [Pg.64]

This equation is coupled to the component balances in Equation (3.9) and with an equation for the pressure e.g., one of Equations (3.14), (3.15), (3.17). There are A +2 equations and some auxiliary algebraic equations to be solved simultaneously. Numerical solution techniques are similar to those used in Section 3.1 for variable-density PFRs. The dependent variables are the component fluxes , the enthalpy H, and the pressure P. A necessary auxiliary equation is the thermodynamic relationship that gives enthalpy as a function of temperature, pressure, and composition. Equation (5.16) with Tref=0 is the simplest example of this relationship and is usually adequate for preliminary calculations. [Pg.164]

The solution of Equations (5.23) or (5.24) is more straightforward when temperature and the component concentrations can be used directly as the dependent variables rather than enthalpy and the component fluxes. In any case, however, the initial values, Ti , Pi , Ui , bj ,... must be known at z = 0. Reaction rates and physical properties can then be calculated at = 0 so that the right-hand side of Equations (5.23) or (5.24) can be evaluated. This gives AT, and thus T z + Az), directly in the case of Equation (5.24) and imphcitly via the enthalpy in the case of Equation (5.23). The component equations are evaluated similarly to give a(z + Az), b(z + Az),... either directly or via the concentration fluxes as described in Section 3.1. The pressure equation is evaluated to give P(z + Az). The various auxiliary equations are used as necessary to determine quantities such as u and Ac at the new axial location. Thus, T,a,b,. .. and other necessary variables are determined at the next axial position along the tubular reactor. The axial position variable z can then be incremented and the entire procedure repeated to give temperatures and compositions at yet the next point. Thus, we march down the tube. [Pg.165]

The time derivatives are dropped for steady-state, continuous flow, although the method of false transients may still be convenient for solving Equations (11.11) and (11.12) (or, for variable Kh, Equations (11.9) and (11.10) together with the appropriate auxiliary equations). The general case is somewhat less complicated than for two-phase batch reactions since system parameters such as V, Vg, Vh and At will have steady-state values. Still, a realistic solution can be quite complicated. [Pg.390]

From what has been said above another conclnsion can be drawn in this direction the po.ssible applications of the implicit scheme (6) in solving the original equation Au = / are equivalent to the numerical. solution of the auxiliary equation Cv = through the use of the explicit scheme... [Pg.681]

As noted in the Introduction, one of the defining characteristics of any fuel-cell model is how it treats transport. Thus, these equations vary depending on the model and are discussed in the appropriate subsections below. Similarly, the auxiliary equations and equilibrium relationships depend on the modeling approach and equations and are introduced and discussed where appropriate. The reactions for a fuel cell are well-known and were introduced in section 3.2.2. Of course, models modify the reaction expressions by including such effects as mass transfer and porous electrodes, as discussed later. Finally, unlike the other equations, the conservation equations are uniformly valid for all models. These equations are summarized below and not really discussed further. [Pg.451]

The technique of chiral auxiliaries was exploited in a synthesis of cholesterol absorption inhibitors, based on an imino-Reformatsky reaction between bromoacetates of chiral alcohols (e.g. 69a and 69b) and imine 70. Virtual complete asymmetric induction was found with (-)-trans-2-phenylcyclohexanol and (—)-phenyl substituted menthol derived chiral auxiliaries (equation 43)126. [Pg.823]

This quadratic equation in 5 is called the auxiliary equation. If its roots are and then the general solution of (1.94) is... [Pg.264]

Dave, J.V. (1964) Meaning of successive iteration of the auxiliary equation in the theory of radiative transfer, Astrophys. J., 140, pp. 1292-1303. [Pg.298]

To solve the differential equation 2.38 subject to the boundary conditions 2.39 and 2.41 we adopt the standard method of substituting the trial solution C — Aemi and obtain the auxiliary equation ... [Pg.99]

If there is no inter-particle interactions out of contact (V = 0), then the auxiliary equation (3.16) takes the simplest form... [Pg.115]

This equation accounts for the decay of the excited state with the rate 1/t a ignored by equation (3.91). The difference between these equations retains when they turn to the auxiliary equations for IET and DET by appending diffusional terms to the rhs of them. However, the usage of the auxiliary equations in these theories is also different one of them is designed for the memory function of IET and another, for the time-dependent rate constant of DET. In spite of all these differences, the results of DET and IET were shown to be identical in the case of irreversible transfer [124],... [Pg.153]

This quantity obeys the auxiliary equation that describes the evolution of the mobile reaction pair during the encounter ... [Pg.155]

The auxiliary equations for the dyads of pair distributions V3, p3 and V2, p2 3X6 the same... [Pg.158]

The global structure of IET formalism is similar to that of DET. The integral kinetic equations substitute for their differential analogs. The kernels of these equations are defined by the transfer rates and pair distribution functions. The auxiliary equations for these functions are also similar but not identical to those in DET. In the next section we will see that the integral theory may sometimes be reduced to the differential one, albeit under rigid conditions and with some losses. [Pg.158]

If there are no reactions in the whole space except those at contact, the transfer terms can be excluded from the auxiliary equations (3.117) ... [Pg.158]

Since it is essentially the same as its intermolecular analog, the definitions of the kernels (3.116) as well as the auxiliary equations (3.117) do not change. Only the integral equations become different ... [Pg.170]

The auxiliary equations for pair correlation functions also differ from previous ones in the very same respect ... [Pg.243]


See other pages where Equation auxiliary is mentioned: [Pg.64]    [Pg.64]    [Pg.71]    [Pg.633]    [Pg.101]    [Pg.109]    [Pg.264]    [Pg.641]    [Pg.283]    [Pg.292]    [Pg.622]    [Pg.294]    [Pg.101]    [Pg.109]    [Pg.64]    [Pg.64]    [Pg.107]    [Pg.120]    [Pg.154]    [Pg.159]    [Pg.171]    [Pg.175]    [Pg.177]    [Pg.204]    [Pg.244]    [Pg.265]    [Pg.285]   
See also in sourсe #XX -- [ Pg.44 ]

See also in sourсe #XX -- [ Pg.213 ]




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