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Fig. 7. Schematic description of a polysiloxane at the monolayer—substrate surface (4). The arrow points to an equatorial Si—O bond that can be connected either to another polysiloxane chain or to the surface. The dashed line on the left is a bond in a possible precursor trimer where the alkyl chains can occupy... Fig. 7. Schematic description of a polysiloxane at the monolayer—substrate surface (4). The arrow points to an equatorial Si—O bond that can be connected either to another polysiloxane chain or to the surface. The dashed line on the left is a bond in a possible precursor trimer where the alkyl chains can occupy...
FIG. 1 Schematic description of the relevant steps involved in a surface catalyzed reaction within the reactive regime. The cycle starts with the empty sites of the surface (top) and is followed by interactions between reactants and the surface (right branch). Such interaction finally leads to the reaction (bottom) and desorption of the products (left branch), a process which generates new empty sites (top). [Pg.389]

Figs. 70, 71 and 72 show schematic descriptions of the three latter above-listed methods. The main advantages and disadvantages of the methods were discussed in general by Volkov and Yazimirsky [294], for all types of molten salts. Regarding the application of the above-mentioned techniques in the investigation of molten fluorides, the following points should be mentioned. [Pg.168]

In Section I, a qualitative schematic description of the main connection between increased agitation intensity and increased total mass-transfer rate was given. It can readily be seen from this description that further research in gas and liquid flow patterns and in the area of relative bubble velocities in dispersions will contribute to the basic knowledge necessary for understand ing the real mechanisms occurring in these systems. [Pg.317]

FIGURE 2.2. A schematic description of the evaluation of the transmission factor F. The figure describes three trajectories that reach the transition state region (in reality we will need many more trajectories for meaningful statistics). Two of our trajectories continue to the product region XP, while one trajectory crosses the line where X = X (the dashed line) but then bounces back to the reactants region XR. Thus, the transmission factor for this case is 2/3. [Pg.45]

FIGURE 2.4. A schematic description of the Langevin Dipole model. The figure illustrates the three steps involved in constructing the model. [Pg.50]

FIGURE 3.3. A schematic description of the two low-energy resonance structures used to describe the S.v2 reaction [see eq. (3.26) for more details]. [Pg.86]

FIGURE 3.9. A schematic description of the free-energy functionals at the range where AG0 > a. [Pg.94]

FIGURE 4.7. A schematic description of the different contributions to the PDLD model. The figure considers the energetics of an ion pair inside a protein interior. The upper part describes the protein permanent dipoles, the middle part describes the induced dipoles of the protein, while the lower part describes the surrounding water molecules and the bulk region, which is represented by a macroscopic continuum model. [Pg.124]

FIGURE 6.2. A schematic description of the rate-determining steps in the catalytic reaction of lysozyme. [Pg.155]

A schematic description of the three-stage process of step reactions is given in Figure 1 and further explained below. [Pg.214]

Figure 4. Schematic description of the swelling process. The molecules of the swelling liquid start to penetrate inside the polymer framework from its surface (a) and to solvate the polymer chains. The polymer chain start to stretch out and to move away from one another the apparent volume of the polymer increases and the first nanopores are formed (b). Swelling stops when increasing elastic forces set up by the unfolding of the polymer chains counterbalance the forces which drive the molecules of the swelling agent into the polymer framework (c). Figure 4. Schematic description of the swelling process. The molecules of the swelling liquid start to penetrate inside the polymer framework from its surface (a) and to solvate the polymer chains. The polymer chain start to stretch out and to move away from one another the apparent volume of the polymer increases and the first nanopores are formed (b). Swelling stops when increasing elastic forces set up by the unfolding of the polymer chains counterbalance the forces which drive the molecules of the swelling agent into the polymer framework (c).
Figure 5. Schematic description of a multi-technique approach to the assessment of molecular mobility inside swollen polymeric frameworks as a phenomenon dependent on their morphology at the nanometric scale [14, 21, 22, 108]. Figure 5. Schematic description of a multi-technique approach to the assessment of molecular mobility inside swollen polymeric frameworks as a phenomenon dependent on their morphology at the nanometric scale [14, 21, 22, 108].
Fig. 1. Schematic description of colloidal metal-catalysed reductions by free radicals... Fig. 1. Schematic description of colloidal metal-catalysed reductions by free radicals...
Figure 1. Schematic description of the low-pressure inductively coupled rf plasma CVD system. Adapted with permission from [33], K. Okada et al., J. Mater. Res. 14, 578 (1999). 1999, Materials Research Society. Figure 1. Schematic description of the low-pressure inductively coupled rf plasma CVD system. Adapted with permission from [33], K. Okada et al., J. Mater. Res. 14, 578 (1999). 1999, Materials Research Society.
Fig. 3.4.1 Schematic description of the three-dimensional SPI technique. Gz, Cx and Gy are the phase encode magnetic field gradients and are amplitude cycled to locate each /(-space point. A single data point is acquired at a fixed encoding time tp after the rf excitation pulse from the free induction decay (FID). TR is the time between excitation (rf) pulses. Notice that the phase encode magnetic field gradients are turned on for the duration of the /(-space point acquisition. Fig. 3.4.1 Schematic description of the three-dimensional SPI technique. Gz, Cx and Gy are the phase encode magnetic field gradients and are amplitude cycled to locate each /(-space point. A single data point is acquired at a fixed encoding time tp after the rf excitation pulse from the free induction decay (FID). TR is the time between excitation (rf) pulses. Notice that the phase encode magnetic field gradients are turned on for the duration of the /(-space point acquisition.
Fig. 3.4.4 Schematic description of the one-dimensional double half k (DHK) SPRITE technique. The phase encode magnetic field gradient, Gz, ramped through half of /(-space beginning at the center and a single data point is acquired at a fixed time (tp) after the rf excitation pulse. The second half of /(-space is acquired after a 5T time delay. The time between rf pulses is TR. Fig. 3.4.4 Schematic description of the one-dimensional double half k (DHK) SPRITE technique. The phase encode magnetic field gradient, Gz, ramped through half of /(-space beginning at the center and a single data point is acquired at a fixed time (tp) after the rf excitation pulse. The second half of /(-space is acquired after a 5T time delay. The time between rf pulses is TR.
Figure 1. Schematic description of organ-specific immunoliposomes. Figure 1. Schematic description of organ-specific immunoliposomes.
Reservoir devices, as the name implies, are characterized by a core of drug, the reservoir, surrounded by a polymeric membrane. The nature of the membrane determines the rate of release of drug from the system. A schematic description of this process is given in Fig. 4, and characteristics of the system are listed in Table 3. [Pg.509]

Schematic description of polymer degradation in the presence of oxygen. Schematic description of polymer degradation in the presence of oxygen.
Figure 3.77 (a) The cycloaliphatic monomer subunits employed by Wegner and Riihe (1989). n varied between 3 and 10. (b) Schematic description of the poly pyrrole backbone wrapped in a layer of poorly conducting methylene moieties of the alkylcne chains fused to the pyrrole units in the 3,4 positions. The minimum separation distance, R, between adjacent chains can be estimated from molecular models. From Wegner and Riihe (1989). [Pg.345]

FIGURE 15.8 Schematic description of layer-by-layer assembly of CNTs with PDDA on the GC surface. [Pg.494]

FIGURE 15.15 Schematic description of the fabrication of multilayer films of GOx onto CNTs. [Pg.502]

Figure 7. (a) Schematic descriptions of the Huang-Rhys factor and the Franck-Condon factors... [Pg.13]

Fig-l- Schematic description of the different zones in an SMB system and the adsorption and desorption processes in these zones... [Pg.213]

Fig. 2. Second-order contributions to intermolecular perturbation energies (schematic description by orbital excitations within the framework of the independent particle model AEpol and zI-Echt are represented by single excitations, AEms by correlated double excitations)... Fig. 2. Second-order contributions to intermolecular perturbation energies (schematic description by orbital excitations within the framework of the independent particle model AEpol and zI-Echt are represented by single excitations, AEms by correlated double excitations)...
Figure S.6. Schematic representation of So and Si energy profiles for DEWAR formation in TB9A and TB9ACN. 2 The excited state funnel F is very close to the ground stale surface and therefore leads to fluorescence quenching (identifiable with rate constant k). Most of the molecules return to the anthracene form via pathway a, while only a few proceed to the Dewar form (pathway b), because F is placed to the left of the ground state barrier. The steric effect of the tert-butyl substituent is indicated by the broken line. Without this prefolding" of the anthracence form. Dewar formation is not observed. The top part of the figure contains a schematic description of the butterfly-type folding process, while the bottom part contains examples of actual molecules. Figure S.6. Schematic representation of So and Si energy profiles for DEWAR formation in TB9A and TB9ACN. 2 The excited state funnel F is very close to the ground stale surface and therefore leads to fluorescence quenching (identifiable with rate constant k). Most of the molecules return to the anthracene form via pathway a, while only a few proceed to the Dewar form (pathway b), because F is placed to the left of the ground state barrier. The steric effect of the tert-butyl substituent is indicated by the broken line. Without this prefolding" of the anthracence form. Dewar formation is not observed. The top part of the figure contains a schematic description of the butterfly-type folding process, while the bottom part contains examples of actual molecules.
Fig.1. Schematic description of dendritic polymers comprising dendrimers and hyper-branched polymers... Fig.1. Schematic description of dendritic polymers comprising dendrimers and hyper-branched polymers...
Fig. 3. Schematic description of self-condensing vinyl polymerization used for the synthesis of of hyperbranched polymers based on vinyl monomers as presented by Frechet [52] -(represents a reactive site which can initiate polymerization)... Fig. 3. Schematic description of self-condensing vinyl polymerization used for the synthesis of of hyperbranched polymers based on vinyl monomers as presented by Frechet [52] -(represents a reactive site which can initiate polymerization)...
Figure 6.1. (a) Three different arrangements of four identical subunits linear, square, and tetrahedral. Their corresponding PFs may be constructed from Table 6.1. (b) Schematic description of the distances (in A) between the four subunits of hemoglobin, in two conformational states. [Pg.194]

Figure 9.4. Schematic description of the solute-solvent pair potential. The double-arrowed line indicates the hard (repulsive) interaction between a and a water molecule. The dashed lines indicate the interaction between groups on the surface of a and a water molecule, the sum of which is the last term on the rhs of Eq. (9.4.1). Figure 9.4. Schematic description of the solute-solvent pair potential. The double-arrowed line indicates the hard (repulsive) interaction between a and a water molecule. The dashed lines indicate the interaction between groups on the surface of a and a water molecule, the sum of which is the last term on the rhs of Eq. (9.4.1).
Figure 2. Whole-Pattern symmetries. Experimental pattern (a) and schematic description of the ten possible Whole Pattern symmetries (b). Figure 2. Whole-Pattern symmetries. Experimental pattern (a) and schematic description of the ten possible Whole Pattern symmetries (b).
Figure 4. Dark-Field symmetries. Experimental patterns (a, b) and schematic description of the five possible Dark-Field symmetries with corresponding symmetry elements (cXfrom... Figure 4. Dark-Field symmetries. Experimental patterns (a, b) and schematic description of the five possible Dark-Field symmetries with corresponding symmetry elements (cXfrom...

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See also in sourсe #XX -- [ Pg.145 ]

See also in sourсe #XX -- [ Pg.204 , Pg.206 ]

See also in sourсe #XX -- [ Pg.145 ]




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High schematic description

Schematic description of the dissociation channels Br(3Pj) H(2S)

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