Reproducibility parallelization

It was not certain that the aquation product would be identical in spectrum to that obtained by thermal reaction, and analysis was therefore carried out chromatographically, rather than spectrophotometrically. The procedure was that described by Woldbye, highly standardized to ensure maximum reproducibility. Parallel separations were carried out on unirradiated solutions, and the chromatographic yields of the cis and trans were in some cases determined by using Cr5i... 

Figure C2.3.12. Two-dimensional neutron scattering by EOggPO gEOgg (Pluronic F88) micellar solution under shear witli (a) tlie sample shear axis parallel to tlie beam, and (b) tlie sample rotated 35° around tlie vertical axis. Reflections for several of tlie Miller indices expected for a bee lattice are annotated. Reproduced by pennission from figure 4 of [84]-...

Compression tests, in which agglomerates ate cmshed between parallel platens, ate probably most universal. To obtain reproducible and accurate results, the rate of loading and method of load appHcation must be strictly controUed. A variety of commercial testers ate available to allow this needed control over the compression process. Several means of distributing the load uniformly at the point of contact ate used, including covering the platen... 

Although fluidized sand or alumina can also be used in the jacket of these somewhat larger reactors, the size makes the jacket design a problem in itself, hence these reactors are seldom used. An advantage of the jacketed reactor is that several—usually four—parallel tubes can be placed in the same jacket. These must be operated at the same temperature, but otherwise all four tubes can have different conditions if needed. This type of arrangement saves time and space in long-lasting catalyst life studies. Jacketed tubular reactors come close, but still cannot reproduce industrial conditions as needed for reliable scale-up. Thermosiphon reactors can be used on all but the most exothermic and fast reactions. 

Figure 15.8. Light transmission of acrylic polymer (5 in thick moulded Diakon. Parallel light beam normally incident on surface). (Reproduced by permission of ICI)...

FIGURE 7A4 Schemes of room ventilation with parallel jet supplied from the same wall (o), from opposite walls (b), and in a fan-type manner (c). Reproduced from Baharev and Troyanovsky. ... 

FIGURE 7.45 Room ventilation by parallel jets. Reproduced from Regenschelt. (1975)... 

Macchi et al. [9] made an extensive study of water injection cycles in their two classic papers and their results are worth a detailed study. Some of their calculations (for ISTIG, RWI and HAT) are reproduced in Figs. 6.18-6.20, all for surface intercooling (parallel calculations for evaporative intercooling are given in the original papers). 

Several sections of the diffraction space of a chiral SWCNT (40, 5) are reproduced in Fig. 11. In Fig. 11(a) the normal incidence pattern is shown note the 2mm symmetry. The sections = constant exhibit bright circles having radii corresponding to the maxima of the Bessel functions in Eq.(7). The absence of azimuthal dependence of the intensity is consistent with the point group symmetry of diffraction space, which reflects the symmetry of direct space i.e. the infinite chiral tube as well as the corresponding diffraction space exhibit a rotation axis of infinite multiplicity parallel to the tube axis. 

The variation of o,.jj with trap depth is presented in Figure 12-19. The effect of traps on the mobility, reflected in an increase of acjj, becomes noticeable only above a certain critical trap depth that depends on concentration. Above that critical value, a2,.), increases approximately linearly with ,. Figure 12-20 shows complementary information concerning the effect of the trap concentration on a,. at constant trap depth. The data reproduces as a family of parallel straight lines on a (Pr/jlo)2 versus In c plot. Their intersection with the ov)jla— 1 tine indicates the critical concentration c, of traps of depth , needed to effect the mobility (see Fig. 12-21). 

The ACS Symposium Series was founded in 1974 to provide a medium for publishing symposia quickly in book form. The format of the Series parallels that of the continuing Advances in Chemistry Series except that in order to save time the papers are not typeset but are reproduced as they are submitted by the authors in camera-ready form. Papers are reviewed under the supervision of the Editors with the assistance of the Series Advisory Board and are selected to maintain the integrity of the symposia however, verbatim reproductions of previously published papers are not accepted. Both reviews and reports of research are acceptable since symposia may embrace both types of presentation. 

The rapid rise in computer speed over recent years has led to atom-based simulations of liquid crystals becoming an important new area of research. Molecular mechanics and Monte Carlo studies of isolated liquid crystal molecules are now routine. However, care must be taken to model properly the influence of a nematic mean field if information about molecular structure in a mesophase is required. The current state-of-the-art consists of studies of (in the order of) 100 molecules in the bulk, in contact with a surface, or in a bilayer in contact with a solvent. Current simulation times can extend to around 10 ns and are sufficient to observe the growth of mesophases from an isotropic liquid. The results from a number of studies look very promising, and a wealth of structural and dynamic data now exists for bulk phases, monolayers and bilayers. Continued development of force fields for liquid crystals will be particularly important in the next few years, and particular emphasis must be placed on the development of all-atom force fields that are able to reproduce liquid phase densities for small molecules. Without these it will be difficult to obtain accurate phase transition temperatures. It will also be necessary to extend atomistic models to several thousand molecules to remove major system size effects which are present in all current work. This will be greatly facilitated by modern parallel simulation methods that allow molecular dynamics simulations to be carried out in parallel on multi-processor systems [115]. 

To examine the details of the structure of flames in channels under quenching conditions, numerical methods were used. Two-dimensional CFD simulation of a propane flame approaching a channel between parallel plates was carried out using the FLUENT code [25]. The model reproduced the geometry of the real channels investigated experimentally. Close to the quenching limit, the burning velocity, dead space, and radius of curvature of the flames were all close to the experimental values. 

Fig. 30 Model for the self-assembly of structure 2 into a double helix comprised of two ribbons, each of which consists of two parallel sheets. Reproduced with permission from Jahnke et al. [70].

Fig. 1 (a) Side and (b) top view of a parallel two-stranded coiled-coil based on heptad sequence repeat (abcdefg). Residues at positions a, d, e and g form the interface between a-helices in a coiled coil stmcture. Prime notations are used to distinguish analogous positions in the two helices fOT example, a and d are analogous positions. Reproduced from Fong et al. [73] licensee BioMed Central Ltd. copyright 2004 (http //genomebiology.eom/2004/5/2/Rll)... 

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