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Manifold scaling

The size-dependence of the intensity of single shake-up lines is dictated by the squares of the coupling amplitudes between the Ih and 2h-lp manifolds, which by definition (22) scale like bielectron integrals. Upon a development based on Bloch functions ((t>n(k)), a LCAO expansion over atomic primitives (y) and lattice summations over cell indices (p), these, in the limit of a stereoregular polymer chain consisting of a large number (Nq) of cells of length ao, take the form (31) ... [Pg.88]

As the physical scale of a reactor increases by numbering up more channels, the micromanifold challenge increases. Fluid distribution occurs in multiple dimensions within a layer [15, 16], from one layer to another [17], and from one reactor to another [18]. An external manifold, also known as the macromanifold or tube connection, as shown in Figure 11.2a, brings the fluids from inlet pipes to the many parallel layers in medium- to large-capacity reactors. [Pg.242]

Several methods have been developed to determine the chemical shift anisotropies in the presence of small and large quadrupolar broadenings, including lineshape analysis of CT or CT plus ST spectra measured under static, MAS, or high-resolution conditions [206-210]. These methods allow for determination of the quadrupolar parameters (Cq, i)q) and chemical shift parameters (dcs, //cs> <5CT), as well as the relative orientation of the quadrupolar and chemical shift tensors. In this context, the MQMAS experiment can be useful, as it scales the CSA by a factor of p in the isotropic dimension, allowing for determination of chemical shift parameters from the spinning sideband manifold [211],... [Pg.164]

An example of a smart tabulation method is the intrinsic, low-dimensional manifold (ILDM) approach (Maas and Pope 1992). This method attempts to reduce the number of dimensions that must be tabulated by projecting the composition vectors onto the nonlinear manifold defined by the slowest chemical time scales.162 In combusting systems far from extinction, the number of slow chemical time scales is typically very small (i.e, one to three). Thus the resulting non-linear slow manifold ILDM will be low-dimensional (see Fig. 6.7), and can be accurately tabulated. However, because the ILDM is non-linear, it is usually difficult to find and to parameterize for a detailed kinetic scheme (especially if the number of slow dimensions is greater than three ). In addition, the shape, location in composition space, and dimension of the ILDM will depend on the inlet flow conditions (i.e., temperature, pressure, species concentrations, etc.). Since the time and computational effort required to construct an ILDM is relatively large, the ILDM approach has yet to find widespread use in transported PDF simulations outside combustion. [Pg.331]

Note that the dimensions of the fast and slow manifolds will depend upon the time step. In the limit where At is much larger than all chemical time scales, the slow manifold will be zero-dimensional. Note also that the fast and slow manifolds are defined locally in composition space. Hence, depending on the location of 0q], the dimensions of the slow manifold can vary greatly. In contrast to the ILDM method, wherein the dimension of the slow manifold must be globally constant (and less than two or three ), ISAT is applicable to slow manifolds of any dimension. Naturally this flexibility comes with a cost ISAT does not reduce the number (Ns) of scalars that are needed to describe a reacting flow.168... [Pg.334]

EPR studies showed that RsSi radicals (R = Me, Et, i-Pr and t-Bu), obtained by hydrogen abstraction from the parent silanes by photogenerated t-BuO radicals, add to Ceo to form the corresponding adducts [29], The spectra of MesSi- and t-Bus Si-adducts have hyperfine structure due to 9 and 27 equivalent protons, respectively, at 27 °C suggesting free rotation of Si—C bonds on the EPR time scale. On the other hand, the middle members of the series, EtsSi-and z-Pr3 Si-adduct radicals, showed a unexpected hyperfine manifold which has been accommodated with free rotation about the Si—Ceo and frozen rotation about the Si—R bonds on the EPR time scale. [Pg.199]

A freeze-dryer must be purchased that either has a large built-in chamber, or to which a chamber can be attached. Some smaller ones are mainly for small-scale work when multiple samples are held in glass flasks or ampoules, which are attached to a manifold equipped with isolation valves. [Pg.20]

In [LJ-control maps the substitution of one ligand by another one results in a change of the range of existence of the manifold intermediates. This change can be expressed by the ligand-property imluced shift of the titration curves identified by the relative position of their inflection points Lq s on the log (lL o/[Ni)Q) scale. These characteristic shifts provide information on the thermodynamic selectivity governed by the association processes only. This type of analysis is designated by . [Pg.99]

B. Oxidation procedure for the small-scale experiments. The required amounts of hexan-l-ol, AA-TEMPO, Mg(N03)2, NBS and HOAc were loaded in the reactor and the flask was connected to the volumetric manifold. The flask was flushed three times with oxygen and immersed in the thermostated water bath held at the reaction temperature for two minutes to equilibrate the system. The oxygen was admitted to the reaction pressure and the continuous monitoring of the oxygen uptake initiated and recorded against the time. After the reaction was completed the product composition was analyzed by GC using dioxane as an internal standard. [Pg.129]

The Holiday Inn was an experiment in cultural technology, making it easy for most people to take long-distance vacations. It helped to change behavior on a large scale, which New York Times writer Walter Kirn says became a ritual whose manifold consequences are unknowable. " ... [Pg.128]

Figure 4.15. Solid-liquid separation in industrial scale using centrifugation in continuous mode (A) or passage of the suspension through manifolds such as those shown in (B) mounted with filter cartridges (C) designed for tangential or cross-flow of liquid suspension. Panel A NIH Fredrick facility, with permission Panels B and C Milipore, MA, with permission. Figure 4.15. Solid-liquid separation in industrial scale using centrifugation in continuous mode (A) or passage of the suspension through manifolds such as those shown in (B) mounted with filter cartridges (C) designed for tangential or cross-flow of liquid suspension. Panel A NIH Fredrick facility, with permission Panels B and C Milipore, MA, with permission.
For P-C-T relationships involving deuterium, a similar procedure was followed. However, studies were limited to the range 0 < D/M 0.01 where D/M represents the deuterium-to-metal atom ratio, and only a 10-Torr, full-scale transducer was used. Deuterium was supplied to the system from a metal deu-teride that was prepared in this laboratory. An alloy of composition TiFeo.gs M11002 (mass 200 g) was activated thoroughly, then outgassed completely at 500° C. The alloy was exposed to deuterium (ultrapure) at 1000 psi for 4 hr, cooled to —196°C, and evacuated. The deuteride reservoir was closed, warmed to room temperature, and moved to the absorption manifold where it served as a high-purity deuterium source. [Pg.356]

There are a number of alternatives and variations to the reduced mechanism method. The intrinsic low dimensional manifold (ILDM) approach [253] and similar methods [399] seek to decouple the fastest time scales in the chemistry. There is a wide range of time scales for chemical reactions in most high-temperature processes, from 10-9 second to seconds. Fast reactions, or reactions with small time scales, quickly bring composition points down to attracting manifolds in the composition space. Then composition points move along on manifolds. In the ILDM approach it is assumed that any movement of the... [Pg.549]

Figure 15.1 shows families of solutions to the model problem for different values of X and different initial conditions. The family of solutions can be thought of as a manifold of solutions, all of which, regardless of the initial condition, tend toward the slowly varying y = t2 + 1 solution. In chemical kinetics, the behavior illustrated in Fig. 15.1 is exhibited by certain species, like the free radicals. After initial very rapid transients such as a combustion ignition, the free-radical concentrations often vary slowly, with their behavior controlled by steady-state or partial-equilibrium conditions. The faster the characteristic scales, the more rapidly the fast-time-constant species come into equilibrium with the major species (i.e., approach a slowly varying solution). [Pg.621]


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See also in sourсe #XX -- [ Pg.166 ]




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Manifolding

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