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Local isotherm

One may choose 6(Q,P,T) such that the integral equation can be inverted to give f Q) from the observed isotherm. Hobson [150] chose a local isotherm function that was essentially a stylized van der Waals form with a linear low-pressure region followed by a vertical step tod = 1. Sips [151] showed that Eq. XVII-127 could be converted to a standard transform if the Langmuir adsorption model was used. One writes... [Pg.656]

Gas A, by itself, adsorbs to a of 0.02 at P = 200 mm Hg, and gas B, by itself, adsorbs tod = 0.02 at P = 20 mm Hg Tisll K in both cases, (a) Calculate the difference between (2a and (2b> the two heats of adsorption. Explain briefly any assumptions or approximations made, ib) Calculate the value for 6 when the solid, at 77 K, is equilibrated with a mixture of A and B such that the final pressures are 200 mm Hg each, (c) Explain whether the answer in b would be raised, lowered, or affected in an unpredictable way if all of the preceding data were the same but the surface was known to be heterogeneous. The local isotherm function can still be assumed to be the Langmuir equation. [Pg.672]

Most calculations of f(Q) for a heterogeneous surface, using an adsorption isotherm assume a patchwise distribution of sites. Explain for what kind of local isotherm functions,/((2,P, T) this assumption is not necessary, and for which it is necessary. Give examples. [Pg.674]

UNIPAJSI. The uniform distribution, Langmuir local isotherm model (9,12) ... [Pg.274]

The adsorption/desorption isotherms measured by NMR (equivalent to conventionally measured isotherms), extracted from two different regions of the imaging field of view corresponding to the two ceramics, are shown in Figure 3.5.9. Once these local isotherms are extracted, they are simply the local adsorption for that point in space contained within the material, measured non-invasively and non-destructively. Conventional analysis techniques for adsorption isotherms (such as BET theory) can therefore be applied to the data, to determine the microstructural properties corresponding to that isotherm curve. [Pg.318]

Nederlof M.M., van Riemsdijk, W.H. and Koopal, L.K. (1990) Determination of adsorption affinity distributions a general framework for methods related to local isotherm approximations./. Coll. Interface Sci., 135, 410-426. [Pg.229]

DFT and Monte Carlo (MC) simulations are modern methods for extracting information on PSDs. Both methods are used for obtaining the local isotherms as functions of pore width and geometry. Knowing the set of local isotherms, the PSDs are obtained by an inverse process solving the GAI equation (Equation 4.28). [Pg.131]

The adsorption isotherm is obtained by relating the chemical potential with the gas bulk density or pressure by using an equation of state. Therefore, the set of local isotherms is obtained by defining the simulation boxes, which describe pores of various widths. [Pg.133]

The NLDFT and GCMC methods can be carried out to obtain a set of local isotherms for pores of different widths. The PSD is obtained by solving the GAI equation (Equation 4.28) in its discrete form ... [Pg.133]

No method has so far been advanced for taking the experimental isotherm itself, irrespective of the complexity of its analytical representation, and from it, obtaining the site energy distribution consistent with any arbitrarily chosen local isotherm function, 0, no matter how complex. [Pg.55]

Our proposed method of site energy distribution analysis can, of course, be applied using any function 0(P,T,Q) for the local isotherm (or even graphical representations not amenable to analytical replication). Nor need the function be explicit in 0. As an example of this last situation, it has been suggested (7) that lateral interaction be allowed for within the framework of the Langmuir approach by supposing Q to increase linearly with 0 ... [Pg.62]

There seem to be no literature data potentially capable of showing definite consistency with Frenkel-Halsey type isotherms, with the exception of the results for nitrogen on titanium dioxide (2). Here we find that no site energy distribution can be constructed using such a local isotherm type which will lead to a fit over the entire range of data. The same appears to be true of local isotherm equations of the polarization theory type ... [Pg.63]

Thus, it is concluded that local isotherm functions of a fairly narrow type such as the Langmuir and Langmuir-plus-lateral interaction types are the rule. Conversely, isotherms of the Frenkel-Halsey and polarization types do not seem applicable in the submonolayer region. [Pg.63]

Rockland (1969) has introduced the concept of local isotherm to provide a closer relationship between sorption isotherms and stability than is possible with other methods. He suggested that the differential coefficient... [Pg.33]

For the moment no transitional states between these extremes will be considered. For these two limiting modes of adsorption the establishment of equilibrium proceeds via different paths in localized adsorption, adsorbed molecules can move to other sites only by desorption and re-attachment, whereas for mobile adsorption the path of tangential transport is also open. Typical representatives of localized isotherms are those of Langmuir. Frumkln-Fowler-Guggen-helm (monolayer) and BET (multilayer). For mobile adsorbates examples are the Volmer and the Hill-De Boer (or two-dimensional Van der Waals) equations. [Pg.76]

The volume V, is that adsorbed on sites or patches having an adsorption energy Ayjj u. The subscript i denotes local in heterogeneity studies the isotherm, describing the adsorption on such homogeneous parts, is often called the local isotherm for which, as already stated, any isotherm equation of app. 1 can be substituted. Volumes pertaining to different local isotherms have to be added in... [Pg.137]

Returning to (1.7.11, it is obvious that, unless additional Information about and/or / is available, a host of isotherms can be predicted by combining certain assumptions regarding the distribution and the local Isotherm, probably enough to "explain" all isotherms ever reported. Suffice it here to give the two illustrations of fig. 1.43(a) and (b). They are taken from Ross and Olivier, who assumed a patchwlse heterogeneous Gauss distribution (see [1.3.7.141) ... [Pg.139]

Figure 1.43. Monolayer adsorption Isotherms on an adsorbent with a Gauss-type energy distribution. After S. Ross and J. P. Olivier, On Physical Adsorption, Interscience Publ. (1964). The local Isotherm is FFG in fig. (a) and Hill-de Boer for lig. (b) (see app. 1). The parameter yis given in (1.7.51. The horizontal scale is adjustable. Figure 1.43. Monolayer adsorption Isotherms on an adsorbent with a Gauss-type energy distribution. After S. Ross and J. P. Olivier, On Physical Adsorption, Interscience Publ. (1964). The local Isotherm is FFG in fig. (a) and Hill-de Boer for lig. (b) (see app. 1). The parameter yis given in (1.7.51. The horizontal scale is adjustable.
Let us finally briefly consider the Inverse problem how to find /(AadgU) if Vlp.T] is known from experiment, and the local isotherm is known (or assumed). Mathematically this procedure is equivalent to solving so-called Fredholm integrals of the first kind the local isotherm functions serve as the kernel. Computationally speaking, this is an ill-posed problem because minor variations in the data may cause substantial variations in /(Aads )- n other words, the Inevitable experimental noise thwarts one obtaining a physically significant distribution. In practice the elaboration may follow one of three paths ... [Pg.141]

The disadvantage of method (i) is that a certain functionality is imposed on an unknown distribution. In approach (il) usually a simplified local isotherm is selected. The distribution function is obtained as a series of derivatives of the... [Pg.141]

From an energetic point of view, the surface of silica is heterogeneous the sur ce is best described by assuming domains corresponding to discrete values of the adsorption energy (defining local isotherms). The sum of the local isotherms reconstructs the observed isotherm. [Pg.889]

Fig. 4 Energy distribution function, (p(s t) (cmol kJ mol ), against the dimensionless product of the lateral interaction energy (P) and the local isotherm (0)P0, for carbon monoxide adsorption over a bimetallic Pto.25-Rho.75 silica-supported catalyst, at 698 K. (From Ref. [12].)... Fig. 4 Energy distribution function, (p(s t) (cmol kJ mol ), against the dimensionless product of the lateral interaction energy (P) and the local isotherm (0)P0, for carbon monoxide adsorption over a bimetallic Pto.25-Rho.75 silica-supported catalyst, at 698 K. (From Ref. [12].)...
Approximation (2) is more straightforward to deal with. We need a theory that accurately describes the local isotherm in either eq. (1) or (2). The classical approach has... [Pg.41]

Density functional theory (DFT) or molecular simulation offer a much more accurate theory for the local isotherm. For simple adsorbates (near-spherical nonpolar molecules) and simple pore geometries (slits, cylinders), DFT is easy to apply, and the results for capillary condensation pressures, and for the remainder of the isotherm, are in... [Pg.42]


See other pages where Local isotherm is mentioned: [Pg.659]    [Pg.867]    [Pg.48]    [Pg.308]    [Pg.178]    [Pg.54]    [Pg.56]    [Pg.62]    [Pg.62]    [Pg.63]    [Pg.63]    [Pg.72]    [Pg.113]    [Pg.113]    [Pg.57]    [Pg.139]    [Pg.140]    [Pg.141]    [Pg.141]    [Pg.123]    [Pg.7]    [Pg.242]    [Pg.41]    [Pg.41]   
See also in sourсe #XX -- [ Pg.26 ]




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