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Chain localization

Although these results need to be understood - and confirmed in other similar systems - the authors claim that they are in qualitative agreement with a model of droplet formation and chain localization resulting from the existence of microscopic heterogeneities within the spinodal boundaries of the phase diagram [256]. [Pg.161]

One of these studies (7) proposed that impact strength arose from a dynamic mechanical dissipation mechanism at the temperature and frequency of the impact. This raises a question whether any one type of loss mechanism (i.e., arising from main chain local mode motions) is better in this respect than another type (i.e., arising from branch motions) as has been proposed (2), or whether the absolute magnitude of the loss at the temperature and frequency of the impact is the criterion. This assessment is the basis of the present study. [Pg.138]

Fibrinogen amyloidosis Variants of fibrinogen a-chain Local... [Pg.1601]

Each local anesthetic molecule has three general areas a lipophilic portion containing an aromatic ring, an intermediate chain and a hydrophilic amine functionality. The structure-activity relationships for local anesthetics can be described in terms of structural modifications to each of these three areas. Depending on the structure of the intermediate chain, local anesthetics are classified as either esters or amides. [Pg.298]

Two kinds of solutions exist, depending on the value of E. Remember that the undisturbed surface local density of states as well as the closed chain local density of states have only a finite density of states if (a—< 40. Solutions of Eq.(2.192a), if they exist, will only be finite in the surface region and will rapidly decline outside the surface region. Since they are outside the band, they can only be satisfied by imaginary values of L in Eki.(2.96). [Pg.91]

For each bath mode, the contribution to the norm from each atom can be calculated from the normalized eigenvectors. Modes with a total contribution larger than 0.5 from the side chain atoms were identified as side chain dominant modes those with a contribution larger than 0.8 from the side chain atoms were identified as side chain localized modes. Similar definitions can be made for porphine core atoms or the two isopropionate groups. Table 9.6 summarizes the results for the dominant modes or the localized modes for those modes involved in the important energy transfer pathways in V4 and V7 modes relaxation. [Pg.218]

Resistance to flow in polymer systems is greater than in low molar mass fluids, because now the molecules are covalently bonded into long chains, which are coiled and entangled, and translational motion must, of necessity, be a cooperative process. It would be unreasonable to expect easy cooperative motion along the entire polymer chain, but as there is normally some degree of flexibility in the chain, local segmental motion can take place more readily. The polymer can then be considered as a sraies of kinetic units each of these moves in an independent manner and involves the cooperative movement of a munber of consecutive chain atoms. [Pg.351]

Multi-structure interpolation methods chain, locally updated planes, self-penalty walk, conjugate peak refinement and nudged elastic band... [Pg.398]

Fig. 17 The mosaic-like structure of crystalline micro-aggregate of EP copolymer chains in the pseudo-hexagonal form, where ordered domains of chains locally arranged as in the orthorhombic-, monoclinic- and triclinic-like model structures of Fig. 15, are assembled together. Long-range positional order of chain axes placed at nodes of a pseudo-hexagonal lattice is maintained. Regions enclosed in a different loop delineate domains of chains ordered in the short-range according to the structural models of Fig. 15... Fig. 17 The mosaic-like structure of crystalline micro-aggregate of EP copolymer chains in the pseudo-hexagonal form, where ordered domains of chains locally arranged as in the orthorhombic-, monoclinic- and triclinic-like model structures of Fig. 15, are assembled together. Long-range positional order of chain axes placed at nodes of a pseudo-hexagonal lattice is maintained. Regions enclosed in a different loop delineate domains of chains ordered in the short-range according to the structural models of Fig. 15...
In the Gaylord-Douglas model [57,81] the chains are localized in a tube defined by the interactions with neighboring chains. The first term of the elastic free energy is the same as that of a phantom network model, while the second term accounts for the loss of degrees of freedom of the chains due to chain localization. In the dry network the cross-sectional dimension of the tube is of the order of the hard-core cross-sectional radius of the polymer chain, and the volume of the tube is comparable with the chain molecular volume. The tube volume is considered to be invariant with macroscopic strain, since the molecular volume of the chains is independent of the deformation. The elastic free energy is given by... [Pg.505]

In conclusion, it can be said that the experiments of Veal et al. and Jorgensen et al. discussed above illustrate clearly the importance of the intra-chain local oxygen ordering. [Pg.37]

If the polymer chain packing is not perfect, interchain disorder will reduce the interchain transfer rate and hence decrease the conductivity. A more realistic model describes heterogeneous polymers. Polymer chains are packed into a bundle and are well ordered inside the bundle. The interchain localization length in the perpendicular direction is Na and the in-chain localization length is M, where / is the localization length in a strictly one-dimensional chain. The state inside these bundles is metallic if localization lengths are high in comparison with lattice constants, Lp > c and > a. The electrical behavior of particular samples is controlled by the dimensions of the bundles. [Pg.140]

Case (B) conesponds to the diffusion-controlled reactions of small molecules with functional groups on polymer side diains. Because the local mode of relaxation of a polymer main chain ( -dispersion) and the rotation of a polymer side diain or phenyl group in the main chain (y-dispersicm) occur below T, the reactions controlled by the side chain local motion begin at temperature correspondmg to the onset of rotational motion and show breals at and T. Quenching or hydrogen abstraction of the benzo d)enone triplet in pofy(methyl methacrylate) may be explained in terms of this idea. [Pg.85]


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See also in sourсe #XX -- [ Pg.20 , Pg.164 , Pg.178 , Pg.191 ]




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Chain configurations, localized

Chains with local correlations (asymptotically Brownian)

Local chain reorientation

Local chain rigidity

Local organisation of polymer chains

Multi-structure interpolation methods chain, locally updated planes, self-penalty walk, conjugate peak refinement and nudged elastic band

NMR studies of local dynamics in side chain thermotropic polymers

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