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Theory multilayer

Multilayer adsorption on heterogeneous surfaces has been analysed in some detail by Jaronlec et al. ). A statistical multilayer theory by Ash et al. ) also deserves special attention. Here the authors considered mixtures of monomers... [Pg.195]

The sigmoidal shape of the nitrogen isotherm of Figure 1 is quite amenable to analyses by the Brunauer-Emmett-Teller (BET) multilayer theory (8). The BET surface area calculated is 2.8 mVg. This value is quite consistent with the predominant l-to-10- xm size distribution observed on this sample with an optical microscope. Assuming cubic habits and density of about 2.3 g/cm, we find the range of specific surface area to be 0.26 to 2.6 m /g. Apparently the sorbed N2 does penetrate into the internal portion of the particles only to a limited extent. [Pg.295]

Ling, G. N. (1979). The polarized multilayer theory of cell water according to the association-induction hypothesis. In Cell-Associated Water (Drost-Hansen, W Clegg, J. S., eds.), pp. 261-269, Academic Press, New York. [Pg.213]

The real advantage of the multilayer theory is, however, that it can utilize both low and high temperature data and in the end give much more reliable values for surface areas. [Pg.230]

The experimental testing of the polarized multilayer theory of cell water involved two steps. In the first step, one tests if the theory has general validity. This requires verifying predictions of the theory in test tubes. If the theory passes this test, then one can proceed to the next step, i.e., to answer the question, Does this theory apply to the living cell The following is a summary of the results of the testing carried out thus far. [Pg.57]

In the present theory of van der Waals adsorption, the multilayer starts below the pressure P and builds up with increasing pressure, and the capillaries are not filled up even for pressures greater than this condensation pressure P, which contradicts the capillary condensation. This means that the multilayer theory based on van der Waals adsorption has an upper limit in the pressure range. Despite this limitation, the van der Waals theory puts all five types of adsorption isotherm shape into one framework, that is it can deal with unimolecular adsorption (Langmuir), multilayer adsorption (BET) and enhanced adsorption in capillaries (BDDT). [Pg.99]

In Table 3.9-1, the range of pore radii is chosen from the lower limit to the upper limit of the mesopore (according to the lUPAC classification, 2 < d < 50 nm). We note that the capillary condensation starts to occur in the smallest mesopore (d = 2 nm = 20 A) at the relative pressure of 0.39. It is reminded here that the upper limit of the relative pressure for the validity of the multilayer theory is about 0.35. This reduced pressure is usually regarded as the demarcation point between the multilayer adsorption and the capillary condensation mechanism, and it is satisfied by many adsorption systems. [Pg.115]

The definition of fCjr and %j Eq. (148) means that the upper limit of integration in Eq. (52) is equal to the saturation pressure, i.e.,/ uj =pQ or/ j.jjj = 1 if Eq. (52) is written in relative pressures. This upper limit of integration corresponds to the supposition that - according to the BET and other multilayer theories - the total mono-layer capacity ( ) is completed at pQ. The proposed name for Eq. (148) is the TM equation. Where m refers to the multilayer adsorption. [Pg.491]

Chemical properties of deposited monolayers have been studied in various ways. The degree of ionization of a substituted coumarin film deposited on quartz was determined as a function of the pH of a solution in contact with the film, from which comparison with Gouy-Chapman theory (see Section V-2) could be made [151]. Several studies have been made of the UV-induced polymerization of monolayers (as well as of multilayers) of diacetylene amphiphiles (see Refs. 168, 169). Excitation energy transfer has been observed in a mixed monolayer of donor and acceptor molecules in stearic acid [170]. Electrical properties have been of interest, particularly the possibility that a suitably asymmetric film might be a unidirectional conductor, that is, a rectifier (see Refs. 171, 172). Optical properties of interest include the ability to make planar optical waveguides of thick LB films [173, 174]. [Pg.560]

W. A. McGahan, and J. A. Woollam. App. Phys. Commun. 9, 1, 1989. Well written and illustrated review of electromagnetic theory applied to a multilayer structure including magnetic and magneto-optic layers. [Pg.411]

In numerous applications of polymeric materials multilayers of films are used. This practice is found in microelectronic, aeronautical, and biomedical applications to name a few. Developing good adhesion between these layers requires interdiffusion of the molecules at the interfaces between the layers over size scales comparable to the molecular diameter (tens of nm). In addition, these interfaces are buried within the specimen. Aside from this practical aspect, interdififlision over short distances holds the key for critically evaluating current theories of polymer difllision. Theories of polymer interdiffusion predict specific shapes for the concentration profile of segments across the interface as a function of time. Interdiffiision studies on bilayered specimen comprised of a layer of polystyrene (PS) on a layer of perdeuterated (PS) d-PS, can be used as a model system that will capture the fundamental physics of the problem. Initially, the bilayer will have a sharp interface, which upon annealing will broaden with time. [Pg.667]

Although still preliminary, the study that provides the most detailed test of the theory for the electronic properties of the ID carbon nanotubes, thus far, is the combined STM/STS study by Oik and Heremans[13]. In this STM/STS study, more than nine individual multilayer tubules with diameters ranging from 1.7 to 9.5 nm were examined. The 7-Fplots provide evidence for both metallic and semiconducting tubules[13,14]. Plots of dl/dV indicate maxima in the ID density of states, suggestive of predicted singularities in the ID density of states for carbon nanotubes. This STM/ STS study further shows that the energy gap for the semiconducting tubules is proportional to the inverse tubule diameter l/<7, and is independent of the tubule chirality. [Pg.32]

In Fig. 10(b) one can see the density profiles calculated for the system with /kgT = 5 and at a high bulk density, p = 0.9038. The relevant computer simulation data can be found in Fig. 5(c) of Ref. 38. It is evident that the theory of Segura et al, shghtly underestimates the multilayer structure of the film. The results of the modified Meister-Kroll-Groot theory [145] are more consistent with the Monte Carlo data (not shown in our... [Pg.216]

This review is structured as follows. In the next section we present the theory for adsorbates that remain in quasi-equilibrium throughout the desorption process, in which case a few macroscopic variables, namely the partial coverages 0, and their rate equations are needed. We introduce the lattice gas model and discuss results ranging from non-interacting adsorbates to systems with multiple interactions, treated essentially exactly with the transfer matrix method, in Sec. II. Examples of the accuracy possible in the modehng of experimental data using this theory, from our own work, are presented for such diverse systems as multilayers of alkali metals on metals, competitive desorption of tellurium from tungsten, and dissociative... [Pg.440]

BET method. The most commonly used method for determining the specific surface area is the so-called BET method, which obtained its name from three Nobel prize winners Brunauer, Emmett and Teller (1938). It is a modification of the Langmuir theory, which, besides monolayer adsorption, also considers multilayer adsorption. The equation allows easy calculation of the surface area, commonly referred to as the BET surface area ( bet). From the isotherms also pore-radii and pore-volumes can be calculated (from classical equation for condensation in the pores). [Pg.100]

Conventional bulk measurements of adsorption are performed by determining the amount of gas adsorbed at equilibrium as a function of pressure, at a constant temperature [23-25], These bulk adsorption isotherms are commonly analyzed using a kinetic theory for multilayer adsorption developed in 1938 by Brunauer, Emmett and Teller (the BET Theory) [23]. BET adsorption isotherms are a common material science technique for surface area analysis of porous solids, and also permit calculation of adsorption energy and fractional surface coverage. While more advanced analysis methods, such as Density Functional Theory, have been developed in recent years, BET remains a mainstay of material science, and is the recommended method for the experimental measurement of pore surface area. This is largely due to the clear physical meaning of its principal assumptions, and its ability to handle the primary effects of adsorbate-adsorbate and adsorbate-substrate interactions. [Pg.305]

Polerecky L., Hamrle J., MacCraith B.D., Theory of the radiation of dipoles placed within a multilayer system, Appl Opt. 2000 39 3968-3977. [Pg.215]

Pidgeon, C., Hunt, A.H., and Dittrich, K. (1986) Formation of multilayered vesicles from water/organic-solvent (W/O) emulsions theory and practice. Pharm. Res. 3, 23-34. [Pg.1103]

A major advance in adsorption theory generalized the treatment of monolayer adsorption and incorporated the concept of multilayer adsorption. This is known as the BET theory after Brunauer, Emmett and Teller [32], The adsorption of a gas on a solid surface can be described by... [Pg.193]

From optical point of view, an OLED structure can be considered as a multilayer thin-film system composed of absorbing and nonabsorbing materials, as shown in Figure 6.27. Therefore, the optical properties and optimal structure of such a multilayer device can be investigated by applying thin-film optical analysis techniques. Based on the theory of optical admittance analysis for analyzing the optical properties of a thin-film system [92], the optical properties of an OLED thin-film system can be simulated to reduce the ambient reflection. [Pg.518]

The other molecular probe method is the single-probe method (SP method), which is separately proposed by Avnir and Jaroniec,93 and Pfeifer et al.108-112 In the SP method, a single adsorption isotherm is analyzed using a modified FHH theory. The FHH model was developed independently by Frenkel,113 Halsey,114 and Hill,115 and describes the multilayer adsorption coverage. Since the SP method uses only one probe molecule, this method is more convenient than the MP method. However, there are many theoretical limitations in applying the SP method to determination of the surface fractal dimension. Therefore, it is really necessary to discuss whether the SP method is an adequate tool to investigate the surface fractal dimension or not before applying the SP method to certain system. [Pg.362]

With this approach we possess the almost complete data-stream and we can look at how the brains of both the receiver and sender actually construct communicative reality. Our approach allows the manipulation of stimuli which can be tested against reality. We will propose a new communication theory which is in its nature multi-modal and multilayered with different channels and many possible communicative principles. [Pg.115]


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See also in sourсe #XX -- [ Pg.203 ]

See also in sourсe #XX -- [ Pg.68 , Pg.69 , Pg.70 ]




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