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Critical binding

Potential allosteric sites that offer additional avenues for drug interactions with functionally critical binding pockets. [Pg.18]

Dual modes of Muncl8-1/SNARE interactions are coupled by 41. functionally critical binding to syntaxin-lN terminus. J. Neurosci. 2007 27 12147-55. 42. [Pg.1258]

Immunoassays are inherently sensitive and specific. However, with continued need to develop increasingly sensitive assays to support preclinical and clinical studies, there have been ongoing efforts to enhance the capabilities of these techniques. Advances in critical binding reagents, detection systems, new assay formats and automation have resulted in improved immunoassay technology. [Pg.1575]

Although most immunoassays have used polyclonal antibodies as the critical binding reagents, development of monoclonal antibodies by Kohler and Milstein in 1975,has resulted in their widespread use, particularly in assays for macromolecules. Their unique epitope specificity conveys advantages in double antibody immunoassays for proteins, where one monoclonal antibody may be used to capture the protein by a specific subunit or epitope, and another, directed against a... [Pg.1575]

Similarly, a chemoenzymatic route was used to generate sLe" -substituted glycopep-tides to elucidate the critical binding epitope of PSGL-1, the physiological ligand for P-selectin (81). In a P-selectin inhibition assay, macrocyclic sLex analog exhibits a dramatic enhancement (100 times) relative to sLe"" (82). [Pg.224]

Fig. 5.10. Comparison between the effective radial potential obtained by Hartree-Fock calculations and a Morse potential adjusted to it. The cases shown are (a) for Ba and (b) for La, while (c) shows the hypergeometric and SCF wavefunctions for case (b). In all the graphs, the full curve is the numerical Hartree-Fock result, while the dotted curves are the Morse fits. The case of Ba is just at the critical binding condition (after J.-P. Connerade [211]). Fig. 5.10. Comparison between the effective radial potential obtained by Hartree-Fock calculations and a Morse potential adjusted to it. The cases shown are (a) for Ba and (b) for La, while (c) shows the hypergeometric and SCF wavefunctions for case (b). In all the graphs, the full curve is the numerical Hartree-Fock result, while the dotted curves are the Morse fits. The case of Ba is just at the critical binding condition (after J.-P. Connerade [211]).
Also starting from the benzylimidazole series reported by the Takeda group, researchers from SmithKline Beecham Pharmaceuticals " - similarly postulated that these compounds were mimicking some of the same, critical binding elements used by All when binding to its receptor. However, the SmithKline Beecham scientists made more extensive use of this hypothesis as part of their design efforts. [Pg.14]

This situation is clearly a manifestation of orbital collapse, and it is therefore no surprise that it occurs for the Q and R the inner well is essentially atomic, and conditions of near-critical binding for the inner well tend to persist from the atom to the solid. If a solid is built up from free atoms with a double-well potential and orbitals in the outer well, the latter hybridize easily, the external part of the orbital going into itinerant states. If one forms a solid from atoms with coUapsed orbitals, then these will remain localized. [Pg.5]

As described in sect. 2, the potential of a free atom from the rare-earth sequence develops two wells. The outer well is the usual atomic well, with an asymptotically coulombic behaviour (long range potential), and contains an infinite number of states. The inner one is a short range well, which is close to the critical binding condition to support one state (4f). This model is backed up by central field self-consistent ab initio Hartree-Fock calculations for free atoms, and involves no adjustable parameters. It correctly describes (a) the order of filling of d and f subshells of the transition elements and R elements (b) the fact that filling occurs deep inside the atom and (c) the behaviour of XAS of free atoms of the Q- and R-element sequences. [Pg.46]

W. R. Garrett, Chem. Phys. Lett., 5, 393-397 (1970). Critical Binding of an Electron to a Non-Stationary Electric Dipole. [Pg.502]


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See also in sourсe #XX -- [ Pg.46 ]




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