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The General Integral Equation

Let us decompose v(x,t),xeC t), as described in Sect. 3.2.4 with the aim of deriving an integral equation for this quantity that is a particular case of the equation given by (2.5.1). We have [Pg.104]


With these kernels, the general integral equations (3.114) take the particular form dedicated to the contact reactions ... [Pg.160]

In the case of great excess of electron acceptors, condition (3.263) remains valid but the generalized integral equations (3.265) accounts for the reversibility of transfer ... [Pg.243]

Equation (16) is the general integral equation from which many multicomponent equilibria models are derived [38,39]. Sircar [40] also used the binary selectivity S instead of energy e in Eq. (16) to study the role of adsorbent heterogeneity in adsorption from a binary liquid mixture. [Pg.412]

When the system consists of a gas mixture containing N components, the overall adsorption equilibrium is described by the general integral equation, Eq. (16). Kapoor et al. applied the extended Langmuir equation as a local isotherm and a uniform energy distribution. The uniform distribution function is... [Pg.425]

The general integral equation (5) for a large, heterogeneous, thermal reactor therefore reduces to the matrix equation... [Pg.15]

The general integral equation (5.28) cannot be solved analytically, therefore one has to look for approximate methods. For two identical plane mirrors of quadratic shape (2a), (5.28) can be solved numerically by splitting it into two one-dimensional equations, one for each coordinate x and y, if the Fresnel number N = a l(dX) is small compared with dld), which means if a < id X) . Such numerical iterations for the infinite strip resonator have been performed by Fox and Li [5.19]. They showed that stationary field configurations do exist and computed the field distributions of these modes, their phase shifts, and their diffraction losses. [Pg.232]

Introduction.— The generalized integral equation for a heterogeneous surface (equation 15) is a linear Fredholm equation of the first kind defined as ... [Pg.6]

This equation is the derivative of the first part of (5.90), so we see that the condition of symmetry for this model leads, via the mean-field approximation for die direct correlation function, to the general integral equation for the profile (4.52). [Pg.158]

Analytical solutions of Eq. (40) are unknown however, Jaroniec etal. [172,173] presented numerical solutions of the general integral equation (40) for a binary gas mixture and for Gaussian and log-normal distributions. [Pg.126]

Because the simplified equation (43) is considerably simpler than the general integral equation (10), it has been used to obtain the analytical adsorption isotherms for mixed-gas adsorption [174-185]. In pioneering works of Roginsky and Todes [178] and Glueckauf [179], the linear relation between adsorption energies was assumed. However, the most intensive studies were performed for the case when the difference between the adsorption energies Sj and , is constant and independent of the type of adsorption site that is... [Pg.127]

The CCSD energy is given by the general CC equation (4.53), and amplitude equations are derived by multiplying (4.50) with a singly excited determinant and integrating (analogously to eq. (4.54)). [Pg.135]

For any transient process that begins at time t and is terminated at a later time tp, the general integral material balance equation has the form... [Pg.334]

Solution An open system extends from —oo to +oo as shown in Figure 9.9. The key to solving this problem is to note that the general solution. Equation (9.18), applies to each of the above regions inlet, reaction zone, and outlet. If k = Q then p=. Each of the equations contains two constants of integration. Thus, a total of six boundary conditions are required. They are... [Pg.333]

The general form of the (RISM) integral equation appropriate for treating solute-solvent interactions which has been derived in the literature is given by " ... [Pg.101]

The intrinsic parameter, characterizing the type of interactions, is the Frumkin interaction parameter a, which is positive for attractive forces and negative for repulsive forces. In addition, 9 = is the fraction of the electrode covered with deposited material, and f ax is the maximal surface coverage. Combining (2.93) and (2.94) with (2.102), the following integral equation is obtained as a general solution ... [Pg.78]

Let us again consider the convolution integral. Equation (86) is an example of a Fredholm integral equation of the first kind. In such equations the kernel can be expressed as a more-general function of both x and x ... [Pg.29]

In terms of heat transfer this can be physically interpreted that, if the infinite heat source is at the boundary (the infinite character is given by the delta function), then for a smooth surface only half of the delta function must be included. The general integral representation of Poisson s equation becomes,... [Pg.518]

The general matrix equation of the problem that determines the amplitudes <2 , (t) is obtained by substitution of the spherical harmonic expansion (4.334) in the Fokker-Planck equation (4.332). After that, the equation is multiplied from the left by X "(e. n)X" (n,h) and, finally, integrated with respect to both e and n. The result can be written in a compact form as... [Pg.562]

The analogy solutions discussed in the previous section use the value of the wall shear stress to predict the wall heat trans er rate. In the case of flow over a flat plate, this wall shear stress is given by a relatively simple expression. However, ir, general, the wall shear stress will depend on the pressure gradient and its variation has to >e computed for each individual case. One approximate way of determining the shear stress distribution is based on the use of the momentum integral equation that was discussed in Chapter 2 [1],[2],[3],[5]. As shown in Chapter 2 (see Eq. 2.172), this equation has the form ... [Pg.272]

Calculate the total number of particles per volume of slurry. This step and the subsequent calculation steps require finding J ° nLjdL, that is (from the equation for n above), 2 x 105/0°°L-,+1 exp (—L/10)dL, where L is as defined above and j varies according to the particular calculation step. From a table of integrals, the general integral is found to be 2 x 105[(y + 1 ) /(l /10y+2]. [Pg.401]

In this later connection, it will be of interest to examine the inhomogeneity correction to the relation (83). To understand the nature of this, we consider the general Euler equation (49). Multiplying this equation by the density p and integrating over the whole of space, yields... [Pg.110]

Their argument for the corrections due to (a) and (b) is briefly summarized below. Correction (c) will be considered in Section 15 and Appendix 4. The inhomogeneity correction (b) above, and the non-zero chemical potential, are both incorporated in the generalized Euler equation (49). Multiplying this by the electron density p and integrating through space yields... [Pg.124]


See other pages where The General Integral Equation is mentioned: [Pg.404]    [Pg.14]    [Pg.246]    [Pg.126]    [Pg.133]    [Pg.104]    [Pg.139]    [Pg.404]    [Pg.14]    [Pg.246]    [Pg.126]    [Pg.133]    [Pg.104]    [Pg.139]    [Pg.52]    [Pg.37]    [Pg.340]    [Pg.241]    [Pg.241]    [Pg.195]    [Pg.61]    [Pg.323]    [Pg.520]    [Pg.323]    [Pg.37]    [Pg.38]    [Pg.98]    [Pg.397]    [Pg.24]   


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