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The Three-Layer Approach

The design of a biorefmery requires the selection of the feedstock type and the valorization processes while keeping the cost low. AU these options introduce the need for a systematic approach for the design of the future biorefmery against haphazard or shortcut choices. The role of a systems approach is to screen chemistries and new processes and to select products and integration scenarios in order to reach a conclusion [Pg.310]

Process integration to target performance with respect to raw material and energy use [Pg.312]

Process flowsheeting for modeling at different levels to evaluate the level of uncertainty in feedstock composition, process chemistries, and costs [Pg.312]

we have to define the problem by developing a process flowsheet. Then, the flowsheets developed can be used to produce scenarios for different feedstock, different products, and detailed costing for CAPEX and OPEX at different scales. The bottom layer can provide every piece of information required by the first layer. Process synthesis is [Pg.312]

Tsakalova and Kokossis (2013) studied the general problem of selecting paths and products from multiple choices and options for the synthesis problem of the aforementioned biorefmery. Their synthesis approach has been applied to select products and paths for  [Pg.313]


In other words the three-layered approach divides a system into active parts treated at a very high level of ab initio molecular orbital theory, a semi-active part that includes important electron contribution and could be treated at a relatively... [Pg.571]

The new system resembles SYNLMA in overall structure we have continued to use the three layered approach. The bottom layer is much like the bottom layer of the old system that is, a custom built theorem prover calling LMA routines to do much of its work. [Pg.120]

Sustainability assessment Figure 12.3 The three-layer approach... [Pg.312]

The standard method of treating the electric dipole contribution from the surface region is to view the nonlinear polarization as a dipole sheet which can be described by the surface susceptibility tensor, xf. This is equivalent to considering the three layer system shown in Fig. 3.1 with the dipole sheet placed just below the surface at z = 0+ and allowing the surface layer thickness, d, to approach zero. The surface contribution to the polarization can then be written as... [Pg.148]

The performance of the cluster approach can be improved dramatically if it is combined with the recently developed ONIOM methodology43 which is an n-layered integrated molecular orbital and molecular mechanics approach. A threelayered version of the ONIOM approximation allows a quantum-mechanical study of systems which are normally considered with molecular mechanics methods to be performed. The three-layered total energy expression for the ONIOM scheme is defined as... [Pg.571]

Figure 24 describes schematically the three recent modes of preparation of membrane/electrode assemblies based on commercially available dispersed platinum catalysts. Comparison of catalyst utilization obtained with the different PEFC catalyzation techniques is given in Fig. 25. The advantage in catalyst utilization of the thin-layer approach is clearly seen, increasing at the higher cell currents (lower cell voltage) thanks to minimized mass-transport limitations in the thin catalyst layer. Figure 24 describes schematically the three recent modes of preparation of membrane/electrode assemblies based on commercially available dispersed platinum catalysts. Comparison of catalyst utilization obtained with the different PEFC catalyzation techniques is given in Fig. 25. The advantage in catalyst utilization of the thin-layer approach is clearly seen, increasing at the higher cell currents (lower cell voltage) thanks to minimized mass-transport limitations in the thin catalyst layer.
The entropy production rate and the complete set of equations that follows can be most conveniently written for the liquid film, the interface, and the vapour film in series.Film layers of thicknesses 5 and in the liquid and the vapour are illustrated in Figure 5. With constant fluxes (in stationary states), the integration is easy. The approach was called the integrated interface approach.For the three layers, the integrated overall force is the sum of the integrated force across each layer ... [Pg.5]

The boundary-layer approach neglects some terms of the momentum equations (3.29) and yields two simplified equations instead of three ... [Pg.103]

The collection of data, that was initially carried out on a voluntary basis, followed a three-layered approach to create a database ... [Pg.100]

In the gas phase, each molecule has three degrees of translational plus two of rotational freedom so that cp iR, plus a small contribution from vibration which will increase to R at higher temperatures. At low temperatures the atoms in the adsorbed layer will be localized and vibrationally unexcited. In this temperature range the isosteric heat therefore increases as iR. As the temperature is raised, however, and surface vibrations begin to contribute, the specific heat of the adatoms will approach that of the gas and finally exceed it, causing a diminution of the heat. This trend reverses once the adsorbed layer approaches the two dimensional gas. Presumably the vibration perpendicular to the surface contributes somewhat before the vibrations in the gas phase become important. The specific heat of the adsorbed layer will therefore continue to exceed that of the gas by a quantity of the order of iR, until all vibrational degrees of freedom are excited and the gas again dominates. [Pg.307]

Table I shows self-diffusion coefficients (T = 300 K) for the three interlayer cations in low-order hydrates of montmorillonite, as calculated conventionally from the slopes of graphs of the (three-dimensional) mean-square cation displacement versus time (8, 16-18). Experimental values of the cation self-diffusion coefficients in aqueous solution also are listed (32). It is apparent that monovalent cation mobility in the one-layer hydrate is at best a few percent of that in bulk aqueous solution, and that the mobility increases significantly with increasing water content, to approach about 25% of the bulk-solution value in the three-layer hydrate. The constrained geometry and the charge sites on the clay mineral surface thus act to retard significantly the diffusive motions of interlayer cations through adsorbed water. Table I shows self-diffusion coefficients (T = 300 K) for the three interlayer cations in low-order hydrates of montmorillonite, as calculated conventionally from the slopes of graphs of the (three-dimensional) mean-square cation displacement versus time (8, 16-18). Experimental values of the cation self-diffusion coefficients in aqueous solution also are listed (32). It is apparent that monovalent cation mobility in the one-layer hydrate is at best a few percent of that in bulk aqueous solution, and that the mobility increases significantly with increasing water content, to approach about 25% of the bulk-solution value in the three-layer hydrate. The constrained geometry and the charge sites on the clay mineral surface thus act to retard significantly the diffusive motions of interlayer cations through adsorbed water.
The approach of multilayering of coarse and fine fibres has also been applied for enhanced drainage functionality. One development is a three-layer non-woven geotextile which is claimed to give a better performance than drainage geocomposites with a geonet core. The three-layer non-woven... [Pg.340]

Sometimes, a highly permeable third layer, e.g., polydimethylsiloxane, is used between the sublayer and toplayer and serves as an intermediate layer or gutter. When the surface of the sublayer is highly porous, it is often difficult to deposit a thin selective coating directly. Also when the toplayer is composed of a glassy polymer it is often difficult to obtain this layer defect-free. Under these circumstances the three-layer membrane or double composite membrane may be a good approach [31]. [Pg.323]

The most important points in this approach is how to present the total energy of all the N layers when each of them is treated differently, how to handle the interface between them, and how to satisfy the condition of interlayer self consistency (Section II). For the energy, the authors suggest the following scheme of calculations. Consider the three-layer system. Denote by, respectively, H, M, and L the high, medium, and low levels of approximation in the calculations, and by S, I, and R the small (central layer), intermediate (central plus next layer), and real (all the three layers) systems, respectively. Then the total energy of the 3-layer system E(3) is presented by the following equation ... [Pg.91]

A second important similarity between the Sustainable Safety and Vision Zero approaches is the shared responsibility of road user and system manager/designer/ operator. Both visions embrace the concept of shared responsibility instead of blaming the victim , as used to be the case in other approaches in the past. Shared responsibility also implies good cooperation between different tiers of the government. This is a component in both visions. In the Netherlands this resnlted in a covenant between the three layers of government with a considerable financial impulse to execute the associated resolutions. [Pg.420]

The three- and four-layered schemes will be examined for two Diels-Alder reactions. The addition of acrolein to 2-t-butyl-1,3-butadiene will be examined with the threelayered ONIOM approach where the model will be taken as ethylene + butadiene, the intermediate model as acrolein 4-isoprene, and the real system as acrolein-f 2-l-butyl-1,3-butadiene. The three ab initio levels of theory will be G2MS CCSD(T)/6-31 G(d) -f MP2/6-311+G(2df,2p) -MP2/6-31G(d), MP4(SDQ), and MP2. This three-layered approach will be extended to a four-layered method by replacing the nine r-butyl hydrogens with methyl groups. This becomes the real system, acrolein -f 2-(trimethyl)-r-butyl-1,3-butadiene, with acrolein-f 2- -butyl-1,3-butadiene as the intermediate large model (int.L.model), acrolein -f isoprene as the intermediate small model (int.S.model), and ethylene-f butadiene as the small model (S.model). The four levels of theory are G2MS, MP4(SDQ), MP2, and HF. The geometry of the transition state and reactants have been optimized... [Pg.1251]

Several independent experimental methods were applied that allowed comparison of the properties of these systems [ 18-20]. We present only the principal results of the three foDowing approaches (i) rheological studies of interfacial adsorption layers (lAL) by the rotating suspension method (ii) observation of the compression of two nonpolar droplets in the surfactant aqueous solution, with measurement of the force needed for their coalescence and (iii) evaluation of the free energy of interaction between nonpolar groups of lAL and various nonpolar liquids by measuring the contact rupture force between two methylated (or fluorinated) smooth solid particles in a given liquid. [Pg.42]

Fig. 1 shows the two-layered profile on a substrate. The quality of reconstruction of this highly contrasted profile is good. The reconstruction of a more complicated three-layered profile on a substrate is shown in Fig. 2. To estimate the robusmess of the approach, a random signal uniformly distributed over the interval [-0.02 +0.02] was added to the real and... Fig. 1 shows the two-layered profile on a substrate. The quality of reconstruction of this highly contrasted profile is good. The reconstruction of a more complicated three-layered profile on a substrate is shown in Fig. 2. To estimate the robusmess of the approach, a random signal uniformly distributed over the interval [-0.02 +0.02] was added to the real and...
This type of coil was prepared from copper cladded printed circuit board material by applying photolithographic techniques. The p.c. board material is available with difierent copper thicknesses and with either a stiff or a flexible carrier. The flexible material offers the opportunity to adapt the planar coil to a curved three dimensional test object. In our turbine blade application this is a major advantage. The thickness of the copper layer was chosen to be 17 pm The period of the coil was 100 pm The coils were patterned by wet etching, A major advantage of this approach is the parallel processing with narrow tolerances, resulting in many identical Eddy current probes. An example of such a probe is shown in fig. 10. [Pg.303]


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