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By heats of immersion

To study the nature and extent of solution adsorption. A small amount of work has been done in studying the interfacial region at solid-solution interface by heat-of-immersion measurements. Few other methods show... [Pg.265]

For simplicity, a systematic classification of solid surfaces by heat of immersion values in a single liquid is desirable. Il in (53) predicted on theoretical grounds a decrease in the heat of wetting with increase in the size of the cation in salts or oxides. However, Il in and Kiselev (54) found that the decrease in the heat of immersion from SrSO< to PbS04 to BaS04 predicted by theory is not observed. Heat data for the immersion of a variety of solids in water are listed in Table VII. Here, too, the changes in heat values are not systematic. [Pg.286]

Solution adsorption studies also deserve to be set apart. A start was made in 1956 by following 1-butanol adsorption out of water onto Graphon by heat of immersion measurements [31]. A model of preferential adsorption of the butanol, plus the measured adsorption isotherm and measured heat effects due to wetting of the adsorbed film at various pertinent concentrations, allowed the heats of immersion to be calculated. Interaction between molecules in the adsorbed film were taken to be the same as in the bulk solution. The calculated values were in excellent agreement with the experimental heats of immersion, as illustrated in Figure 7. No further studies of this kind have been performed on other fimctional groups, different chain lengths, or other molecular structures. [Pg.96]

Okuda, S., K. Inoue, and I. Uei, 1960. Measurement of surface mean diameter of powders by heat of immersion method. Memoirs Fac. Industrial Arts, Kyoto Technical University. Sci. and Tech. 9 61-78. [Pg.526]

The heat of immersion is measured calorimetrically with finely divided powders as described by several authors [9,11-14] and also in Section XVI-4. Some hi data are given in Table X-1. Polar solids show large heats of immersion in polar liquids and smaller ones in nonpolar liquids. Zetdemoyer [15] noted that for a given solid, hi was essentially a linear function of the dipole moment of the wetting liquid. [Pg.349]

A number of methods have been described in earlier sections whereby the surface free energy or total energy could be estimated. Generally, it was necessary to assume that the surface area was known by some other means conversely, if some estimate of the specific thermodynamic quantity is available, the application may be reversed to give a surface area determination. This is true if the heat of solution of a powder (Section VII-5B), its heat of immersion (Section X-3A), or its solubility increase (Section X-2) are known. [Pg.576]

The general type of approach, that is, the comparison of an experimental heat of immersion with the expected value per square centimeter, has been discussed and implemented by numerous authors [21,22]. It is possible, for example, to estimate sv - sl from adsorption data or from the so-called isosteric heat of adsorption (see Section XVII-12B). In many cases where approximate relative areas only are desired, as with coals or other natural products, the heat of immersion method has much to recommend it. In the case of microporous adsorbents surface areas from heats of immersion can be larger than those from adsorption studies [23], but the former are the more correct [24]. [Pg.576]

Make a numerical estimate, with an explanation of the assumptions involved, of the specific surface area that would be found by (a) a rate of dissolving study, (b) Harkins and Jura, who find that at the adsorption of water vapor is 6.5 cm STP/g (and then proceed with a heat of immersion measurement), and (c) a measurement of the permeability to liquid flow through a compacted plug of the powder. [Pg.593]

The heat of adsorption is an important experimental quantity. The heat evolution with each of successive admissions of adsorbate vapor may be measured directly by means of a calorimeter described by Beebe and co-workers [31]. Alternatively, the heat of immersion in liquid adsorbate of adsorbent having various amounts preadsorbed on it may be determined. The difference between any two values is related to the integral heat of adsorption (see Section X-3A) between the two degrees of coverage. See Refs. 32 and 33 for experimental papers in this area. [Pg.616]

The integral heat of adsorption Qi may be measured calorimetrically by determining directly the heat evolution when the desired amount of adsorbate is admitted to the clean solid surface. Alternatively, it may be more convenient to measure the heat of immersion of the solid in pure liquid adsorbate. Immersion of clean solid gives the integral heat of adsorption at P = Pq, that is, Qi(Po) or qi(Po), whereas immersion of solid previously equilibrated with adsorbate at pressure P gives the difference [qi(Po) differential heat of adsorption q may be obtained from the slope of the Qi-n plot, or by measuring the heat evolved as small increments of adsorbate are added [123]. [Pg.647]

Fig. 4.24 Heat of immersion of a carbon (prepared by pyrolysis of Saran Polymer A) in different liquids at 300 K. The liquids for points 1-6 were (I) methanol (2) benzene (3) n-hexane (4) 3-methyl benzene (5) 2,2-dimethyl butane (6) 2,2,4-trimethyl pentane. The abscissae represent the molar volumes of the liquids. (Redrawn from the original diagram of Barton, Beswick and Harrison. " )... Fig. 4.24 Heat of immersion of a carbon (prepared by pyrolysis of Saran Polymer A) in different liquids at 300 K. The liquids for points 1-6 were (I) methanol (2) benzene (3) n-hexane (4) 3-methyl benzene (5) 2,2-dimethyl butane (6) 2,2,4-trimethyl pentane. The abscissae represent the molar volumes of the liquids. (Redrawn from the original diagram of Barton, Beswick and Harrison. " )...
Phtnalic anhydride is made by oxidation of naphthalene at temperatures of 340 to 380°C (644 to 716°F) controlled by heat exchangers immersed in the bed. At these temperatures the catalyst is stable and need not be regenerated. The excellence of temperature control was a major fac tor for the adoption of this process, but it was obsolesced by 1972. [Pg.2104]

Matsuda, H., Ueda, M. and Murakami, K. (1988f). Oligoesterifed woods based upon anhydride and epoxide II. Preparation and dimensional stability of ohgoesterified woods by heating wood immersed in anhydride-epoxide solution. Mokuzai Gakkaishi, 34(7), 597-603. [Pg.216]

Hydrogen is chemisorbed by diamond at temperatures from 400° upwards as was shown by Barrer (134b). Apparently, surface hydrides are formed as is indicated by the decrease in the capacity for potassium chemisorption (Table XIII). A significant decrease was also measured for the heat of immersion in water after hydrogen treatment at 800° [(55), Table XIV]. Methane is liberated when hydride-covered diamond is heated in a vacuum (153c). [Pg.222]

Wade and Hackerman (302) measured the heats of immersion in water of both anatase and rutile as a function of particle size and outgassing temperature. Apart from the distinct influence of the particle size, a maximum in the heat of immersion was observed after outgassing at 300 to 350°, indicating a rehydroxylation reaction. This is similar to the behavior of silica. Whereas, with silica, the decrease at higher evacuation temperatures is caused by the slowness of the reopening of siloxane bonds (see Section III,A,2), it is very probably caused by a decrease in surface area in the case of TiOj. The maximum in the heat of immersion curves was distinct only with samples of high surface area. Stbber et al. (225) observed a decrease in the surface area of fine particle size anatase already at 450°. [Pg.251]

To measure the site energy distribution or other surface properties of powders by measuring heats of immersion as a function of the amount of preadsorbed wetting liquid. Heats of immersion of the partly covered surfaces reveal the site energy distributions. For acid sites on cracking catalysts, for example, adsorbates of different basicity can be used to develop a topographical map of the surface activity. [Pg.265]

Here,, the surface energy of the wetting liquid, and the heat of immersion hn8 ) are the measurable quantities. The quantity is given by the expression ... [Pg.274]

The very low water adsorption by Graphon precludes reliable calculations of thermodynamic quantities from isotherms at two temperatures. By combining one adsorption isotherm with measurements of the heats of immersion, however, it is possible to calculate both the isosteric heat and entropy change on adsorption with Equations (9) and (10). If the surface is assumed to be unperturbed by the adsorption, the absolute entropy of the water in the adsorbed state can be calculated. The isosteric heat values are much less than the heat of liquefaction with a minimum of 6 kcal./mole near the B.E.T. the entropy values are much greater than for liquid water. The formation of a two-dimensional gaseous film could account for the high entropy and low heat values, but the total evidence 22) indicates that water molecules adsorb on isolated sites (1 in 1,500), so that patch-wise adsorption takes place. [Pg.276]

Future important contributions of heats of immersion will be made in the field of solution adsorption despite the necessity for more exacting experimentation. The common problem in solution adsorption has been to define the nature and extent of the interface between solid particles and mixed liquids. Specifically, more information is needed concerning the orientation and solvation of adsorbed molecules as well as the composition and practical boundary of the adsorbed phase. Direct adsorption measurements yield only net changes in concentration and indirect approaches must be taken (66). Much can be learned, however, by measuring the heats of immersion of powders into two component solutions of varying composition where the adsorption of one component is predominant. This technique, also, is the only available method for measuring the heat of adsorption of... [Pg.291]

Another approach to resolving this theoretical objection to Young s equation is to eliminate the difference (ysv — ySL) from the equation entirely, replacing it by some equivalent quantity, thereby shifting attention away from the notion of solid surface tension. An example of this is the use of the heat of immersion to test Young s equation. We return to this in Section 6.6c. [Pg.267]

Small quantities of heat are generally evolved when a dry solid is immersed in a liquid. This can be measured calorimetrically and is called the heat of immersion. The physical process with which this heat is associated may be represented by the following equation ... [Pg.268]

Following the usual thermochemical convention, the heat of immersion AHim may be written Hwe, - Hdry, with these enthalpies expressed per unit area. Since heat is released by this process, AHim is negative. The wet surface clearly describes the SL interface. For the dry surface, we ignore -jre and describe the surface by the 5° notation. Therefore the heat of immersion may also be written... [Pg.268]

FIG. 6.7 Heats of immersion determined by calorimetry and calculated by Equation (54) for Teflon in various alkanes. (Redrawn from A. W. Neumann, Adv. Colloid Interface Sci., 4, 105 (1974).)... [Pg.269]

Colloidal carbon was formed by the slow pyroloysis of polyvinylidene chloride. Surface oxidation occurs during subsequent storage in air. By heating at elevated temperatures, the following gases are evolvedt (heats of immersion were also measured after the different thermal pretreatments) ... [Pg.459]

Using 7.9 and 9.1 A2 as the areas of oxide desorbing as CO and C02, respectively, estimate the area (in m2 g ) occupied by each of these oxide types. If the specific area of the carbon is 1100 m2 g , what percentage of the surface is covered with oxide Discuss the variation of the heat of immersion with the removal of the surface oxides. [Pg.459]


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