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Heavy different structures

So the disparity between intensities of Friedel pairs in the anomalous scattering data set establishes their phases in the nonanomalous scattering data set. The reflection whose phase has been established here corresponds to the vector Fhp in Eq. (6.9). Thus the amplitudes and phases of two of the three vectors in the Eq. (6.9) are known (l)FHp is known from the anomalous scattering computation just shown, and (2) FH is known from calculating the heavy-atom structure factors after locating the heavy atom by Patterson methods. The vector Fp, then, is simply the vector difference establish-... [Pg.123]

Fig. 8.7. Specific surface areas plotted for structured packings are from Table 8.2, and the packing factors are from the manufacturers publications (22,30,31). For structured packings, the packing factors become a function of liquid load when liquid load exceeds about 20 gpm/ft2 (30,31). For this reason, one line (heavy) was drawn for liquid loads lower than 20 gpm/ft2. The points for structured packings at higher liquid loads were connected by dashed lines parallel to the heavy line. Due to these approximations, Fig. 8.12a is unsuitsble for a comparative evaluation among different structured packings. Fig. 8.7. Specific surface areas plotted for structured packings are from Table 8.2, and the packing factors are from the manufacturers publications (22,30,31). For structured packings, the packing factors become a function of liquid load when liquid load exceeds about 20 gpm/ft2 (30,31). For this reason, one line (heavy) was drawn for liquid loads lower than 20 gpm/ft2. The points for structured packings at higher liquid loads were connected by dashed lines parallel to the heavy line. Due to these approximations, Fig. 8.12a is unsuitsble for a comparative evaluation among different structured packings.
Figure 7. A vector diagram illustrating the effects of heavy atom anomalous scattering on the reflections hkl (denoted +) and filci (denoted —). Fpn is the average structure factor amplitude for the heavy atom derivative of the protein. FJ Ih imaginary part of the heavy atom structure factor amplitude which arises from anomalous scattering. Because FJl always advances the phase by fI/2, FpH (+) and Fpn (—) are no longer equal. The measured difference between these amplitudes can be used fbr phase determination. Figure 7. A vector diagram illustrating the effects of heavy atom anomalous scattering on the reflections hkl (denoted +) and filci (denoted —). Fpn is the average structure factor amplitude for the heavy atom derivative of the protein. FJ Ih imaginary part of the heavy atom structure factor amplitude which arises from anomalous scattering. Because FJl always advances the phase by fI/2, FpH (+) and Fpn (—) are no longer equal. The measured difference between these amplitudes can be used fbr phase determination.
Heavy atom derivatives of a macromolecular crystal can be prepared (Green, Ingram and Perutz 1954) which for a minimum of two derivatives (and the native crystal) and in the absence of errors, leads to a unique determination of the phase ahkt in equation (2.7) (figure 2.13(a)). This requires the site and occupancy of the heavy atom to be known for the calculation of the vector FH (the heavy atom structure factor). In the absence of any starting phase information the heavy atom is located using an isomorphous difference Patterson synthesis P(u,v,w) where the isomorphous difference is given by... [Pg.38]

An FAB-MS study on several aromahc, aliphatic, and aliphatic-aromatic polysulfides doped with heavy metal salts allowed the detection of adducts of the cyclic sulfides with heavy metal ions Ag, Hg, and Cu - The molecular ions of the cyclic sulfides and those corresponding to the metal adducts appeared in the spectra with widely differing intensities, providing a tool to investigate the selectivity of metals toward macrocyclic sulfides of different structure and size. ... [Pg.284]

The ternary compounds with the general formula Th2(N,0)2X, where X denotes the heavy elements below row 1 in Columns V and VI of the periodic table, crystallize in two different structure types, a hexagonal and a body-centered tetragonal one. The crystal type assumed depends on the size of the X atom [5]. When X = Sb, Bi, or Te, the X atom can have a... [Pg.46]

Mo or W sulEdes which are promoted by Co, Ni supported on alumina or silica-alumina are practically used in large amounts for hydrodesuliiirization of heavy oil. Structure, properties and catalytic function of these catalysts have been studied extensively. These reactions are not simple acid-base reactions. It has been suggested that there are two different active sites on Mo sulfide coordinatively unsaturated Mo (Lewis acid site) and Brensted acid site induced by the interaction of HjS with Mo... [Pg.183]

So, the ethylene production does correlate with coke presence, in particular with aromatics formation as far as the diffusion limitations are not significant. However, it seems that the majority of ethylene is not always formed directly from MeOH [115]. The aromatics and other coke species could be the products of the conversion of primary carbenium ions, which are mobile and could equilibrate each other [28]. This may explain the isotopic distribution in products and retained coke molecules and the coexistence of aromatics and carbenium ions [28], In addition to the coproduction of ethylene with aromatics in olefins interconversion cycle, formation of ethylene via alkylation-dealkylation of methyl aromatics with heavy olefins or with the equivalent carbenium ions like ethyP, propyP, and butyP could be an option. The alkyl aromatics with the side chain length of two carbons or longer are not stable in the pore and dealkylates on the acid sites due to too long residence time and steric hindrances. This may lead to formation of ethylene, other olefins, and alkylaromatics with different structure, namely PMBs [129]. In other words, the ethylene is formed via interaction of the carbenium ions like ethyP, propyP, and butyP formed from MeOH or heavy olefins with aromatics and other coke precursors followed by cracking and in a less extent by a direct alkylation of PMBs with methanol. The speculation is based properly on analysis of the prior arts and is not contradictory with the concept of the aromatic cycle for ethylene formation. [Pg.222]

When it comes to the heaviest of petroieum fractions, modern analytical methods are not able to isolate and characterize the molecules completely. In the absence of something better, the analyst separates the heavy fractions into different categories, which leads merely to definitions that are workable but are no longer in terms of exact structure. [Pg.13]

The basic structure of all immunoglobulin (Ig) molecules comprises two identical light chains and two identical heavy chains linked together by disulfide bonds (Figure IS.2a). There are two different classes, or isotypes, of light chains, X and k, but there is no known functional distinction between them. Heavy chains, by contrast, have five different isotypes that divide the immunoglobulins into different functional classes IgG, IgM, IgA, IgD, and IgE, each with different effector properties in the elimination of antigen... [Pg.300]


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See also in sourсe #XX -- [ Pg.34 , Pg.35 , Pg.36 , Pg.37 , Pg.38 , Pg.39 , Pg.40 ]




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Structural differences

Structure difference

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