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SOS structures

With numerous —OH groups of similar reactivity, polysaccharides are so. structurally complex that their laboratory synthesis has been a particularly difficult problem. Several methods have recently been devised, however, that have... [Pg.1001]

Figure 17. Internal energy distributions of HCO from photodissociation of CH2O at 2549 cm (upper panel) and 2627 cm (lower panel) above the threshold for the H + HCO channel. The HCO vibrational thresholds are labeled with their quantum numbers, and combs label the stack thresholds. The open circles show predictions of the SSE/PST model. The upper panel is indicative of an So dominant pathway. In the lower panel, T is dominant, but So structure can still be observed. Reprinted with permission from [51]. Copyright 2000, American Institute of Physics. Figure 17. Internal energy distributions of HCO from photodissociation of CH2O at 2549 cm (upper panel) and 2627 cm (lower panel) above the threshold for the H + HCO channel. The HCO vibrational thresholds are labeled with their quantum numbers, and combs label the stack thresholds. The open circles show predictions of the SSE/PST model. The upper panel is indicative of an So dominant pathway. In the lower panel, T is dominant, but So structure can still be observed. Reprinted with permission from [51]. Copyright 2000, American Institute of Physics.
David Hull. My purpose for presenting the wedding-cake model is to indicate how inadequate it is. In my talk, I mentioned that the humanities are being left out of the wedding-cake model. Certainly mathematics is also being left out. I would like to see a model that is so structured that it includes more than just the empirical sciences, narrowly defined. But you are right. Mathematics is crucial to science, and it is omitted from the wedding cake model. [Pg.173]

In this case, even with there being one double bond, the formal charge on the sulfur atom is +2, so structures that show two double bonds are possible, which can reduce further the positive formal charge. In order for structures such as... [Pg.113]

Now we consider thermodynamic properties of the system described by the Hamiltonian (2.4.5) it is a generalized Hamiltonian of the isotropic Ashkin-Teller model100,101 expressed in terms of interactions between pairs of spins lattice site nm of a square lattice. Hamiltonian (2.4.5) differs from the known one in that it includes not only the contribution from the four-spin interaction (the term with the coefficient J3), but also the anisotropic contribution (the term with the coefficient J2) which accounts for cross interactions of spins a m and s m between neighboring lattice sites. This term is so structured that it vanishes if there are no fluctuation interactions between cr- and s-subsystems. As a result, with sufficiently small coefficients J2, we arrive at a typical phase diagram of the isotropic Ashkin-Teller model,101 102 limited by the plausible values of coefficients in Eq. (2.4.6). At J, > J3, the phase transition line... [Pg.44]

The structure of FeRu3(CO)i3H2 is shown in Fig. 10 and the infrared spectrum of the iron/osmium analogue suggests it is /so-structural. [Pg.53]

Diazinothiazines were not discussed in CHEC(1984), but the chemistry of five known diazinothiazine systems was reviewed in CHEC-II(1996) <1996CHEC-II(7)737>. Some older syntheses of diazinothiazines are also included in a recent review . Generally, the only structural data available for diazinothiazines are those acquired in the course of confirming the identity of products, and so structural studies will not be discussed separately. [Pg.1062]

Because electronic and ionic conduction are so structure-sensitive, the simple rule-of-mixtures approach to estimating the conductivity and resistivity of composites is not normally of use. As a result, the conductivity of specific composites for specific applications must be experimentally determined. In the next two sections, we examine two examples of how composites can be used in electrical applications, and we describe the influence of each component on the electrical properties. The first example involves the electrical insulating properties of polymers, and the second one involves enhancing the electrically conducting properties of polymers. [Pg.592]

Transition state analogues are essentially stable molecules which resemble, in geometry and in charge distribution, metastable intermediates of the enzymic reaction. The actual transition state of the reaction will be close in structure to the metastable intermediate, and will quite likely vary slightly between different substrates accepted by the same enzyme. There will not be a unique transition state for all transformations catalysed by one particular enzyme, neither of course will there be a unique transition state for different enzymes catalysing the hydrolysis of peptide links in a protein. There will nevertheless be some similarities in mechanism, and so structures containing a tetrahedral centre have been designed to inhibit a variety of proteinases, where a tetrahedral intermediate is always presumed. Differences exist in the pathway to, and breakdown of, the tetrahedral intermediate, and its stabilization, between thiol and serine proteinases, zinc proteinases, and aspartic proteinases. [Pg.125]

When the action. . . has dire economic or social consequences, the person who must make the decision may be sorely tempted to ask for a reinterpretation of the data. Risk assessment can be like a captured spy If you torture it long enough, it will tell you anything you want to know. So it is good public policy to so structure an agency that such temptation is avoided. [Pg.683]

The first three geometries involve the tetrahedral, trigonal, and digonal hybrids discussed above and the fourth involves the use of pure s and p orbitals as discussed on page 149. The last structure contains three equivalent bonds at mutual angles of 60 and a fourth bond at an angle of approximately 145° to the others. U is impossible to construct s-p hybrid orbitals with angles less than 90°, and so structure V is ruled out. In this sense it may be sard that hybridization does not allow" structure V, but it may not be said that it "chooses ore of the others. Carbon hybridizes sp, sp2, and spJ in various compounds, und the choice of sp3 in methane is a result of the foot that the tetrahedral structure is the most stable possible. [Pg.624]

Progress in zeolite crystallization in the last several years has been mostly in the experimental realm and has resulted in several new synthetic zeolites and compositional variants of previously known structures. Theoretical advances have come more slowly but are significant. Until the elucidation of zeolite structures in the last decade or so, structural interpretation of crystallization phenomena was not possible. As additional physical and chemical techniques are applied to the complex structural chemistry of zeolite crystallization, our understanding of the mechanism increases, and the extent of empiricism in synthesis decreases. Areas of investigation still unexplored that should add considerable understanding... [Pg.139]

The microwave spectrum of the normal argon-acetaldehyde and of the Ar-CHsCDO van der Waals dimer has been used to determine their structure646 which was found to be a non-planar skew, with the Ar binding on top of the C—C—O triangle. The planar or nearly so structure of the Ar-formic acid van der Waals dimer has also been determined647 from assigning the rotation spectrum of normal, Ar, DCOOH and HCOOH isotopomers. [Pg.1080]

Because Fhkl is a periodic function, it possesses amplitude, frequency, and phase. It is a diffracted X ray, so its frequency is that of the X-ray source. The amplitude of Fhkl is proportional to the square root of the reflection intensity lhkl, so structure amplitudes are directly obtainable from measured reflection intensities. But the phase of Fhkl is not directly obtainable from a single measurement of the reflection intensity. In order to compute p(x,y,z) from the structure factors, we must obtain, in addition to the intensity of each reflection, the phase of each diffracted ray. In Chapter 6,1 will present an expression for p(x,y,z) as a Fourier series in which the phases are explicit, and I will discuss means of obtaining phases. This is one of the most difficult problems in crystallography. For now, on the assumption that the phases can be obtained, and thus that complete structure factors are obtainable, I will consider further the implications of Eqs. (5.15) (structure factors F expressed in terms of atoms), (5.16) [structure factors in terms of p(x,y,z)], and (5.18) [p(x,y,z) in terms of structure factors]. [Pg.95]

While not so structurally perfect (see Sections 1.3 and 1.4) as their dendritic relatives, these hyperbranched dendritic compounds (see Section 2.7) can be produced faster and at less expense, making them especially interesting for the materials sector. The various commercially available monomers (Fig. 4.51) offer great structural versatility. [Pg.128]

Another possible application using the hierarchical nature of the wrinkles has been discussed by Efimenko and coworkers [46], They treated a mechanically stretched PDMS sheet with UV-ozone in order to create a stiff surface layer. A detailed analysis with AFM and profilometry of the wrinkles after releasing the strain showed that the wrinkling patterns are hierarchical themselves. They observed up to five generations of different wavelengths with different periodicities. These features made so structured surfaces valuable candidates for separate colloidal particles of different sizes by acting as a micro fluidic sieve. A suspension... [Pg.90]

In summary, we have demonstrated that the concept of a structure-field map is a useful one in systematizing the occurrence of crystal structures in a series of iso-stoichiometric compounds. In addition, the concept of a weighted mean radius of an ion at a particular site in a substituted compound has been found to be a valid one. The use of a SFM to predict structural stability and provide warnings about possible polymorphism (and so structural integrity) in a complex multicomponent substituted system could be a useful tool in assessing potential hosts for nuclear waste isolation. [Pg.303]

Whereas the well-characterized, perfect (or nearly so) structures of dendritic macromolecules, constructed in discrete stepwise procedures have been described in the preceding chapters, this Chapter reports on the related, less than perfect, hyperbranched polymers, which are synthesized by means of a direct, one-step polycondensation of A B monomers, where x > 2. Flory s prediction and subsequent demonstration 1,2 that A B monomers generate highly branched polymers heralded advances in the creation of idealized dendritic systems thus the desire for simpler, and in most cases more economical, (one-step) procedures to the hyperbranched relatives became more attractive. [Pg.165]


See other pages where SOS structures is mentioned: [Pg.90]    [Pg.193]    [Pg.1048]    [Pg.1049]    [Pg.451]    [Pg.35]    [Pg.129]    [Pg.23]    [Pg.61]    [Pg.101]    [Pg.102]    [Pg.100]    [Pg.158]    [Pg.207]    [Pg.208]    [Pg.884]    [Pg.551]    [Pg.48]    [Pg.211]    [Pg.91]    [Pg.85]    [Pg.73]    [Pg.102]    [Pg.103]    [Pg.302]    [Pg.70]    [Pg.196]    [Pg.451]    [Pg.132]    [Pg.55]    [Pg.84]    [Pg.328]   
See also in sourсe #XX -- [ Pg.2 , Pg.486 ]




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