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Interaction with chain

Free-radical chain stoppers—These chemicals interact with chain propagating R02 radicals to form inactive products. [Pg.467]

Classical molecular theories of rubber elasticity (7, 8) lead to an elastic equation of state which predicts the reduced stress to be constant over the entire range of uniaxial deformation. To explain this deviation between the classical theories and reality. Flory (9) and Ronca and Allegra (10) have separately proposed a new model based on the hypothesis that in a real network, the fluctuations of a junction about its mean position may may be significantly impeded by interactions with chains emanating from spatially, but not topologically, neighboring junctions. Thus, the junctions in a real network are more constrained than those in a phantom network. The elastic force is taken to be the sum of two contributions (9) ... [Pg.330]

Olsnes, S., Pappenheimer, A.M., Jr. and Meren, R. (1974a) Lectins from Abrus precatorius and Ricinus communis. II. Hybrid toxins and their interaction with chain-specific antibodies. J Immunol, 113, 842-847. [Pg.462]

It should be considered that at RE conditions when the process is fast in order to provide for a high yield of the grafted product, grafting initiators should be peroxides that show thermodynamic affinity with PO (12,15-18). A higher solubility of a peroxide initiator in a polymer (not in a monomer) leads to the fact that radicals— formed during thermal decomposition of the initiator— first interact with chains. Macroradicals formed initiate the reaction of grafting of the monomer to the chains. [Pg.273]

Peroxide decomposers, which promote the conversion of peroxides to non-free radical products, presumably by a polar mechanism. Examples are dialkylarylphosphites, dialkylthiodipropionates or long chain alkylmercaptans. Free radical chain stoppers or "radical traps," which interact with chain-propagating RO2 radicals to form inactive products. This is usually accomplished by its donation of an H radical to terminate an active polymer radical, itself forming a more stable one (usually by resonance) which will not rereact with the polymer (e.g., with the help of steric hindrance) and will eventually relax its energy through thermalization, fluorescence or other innocuous means. Examples are sterically hindered phenols or secondary arylamines. [Pg.391]

We will describe integral equation approximations for the two-particle correlation fiinctions. There is no single approximation that is equally good for all interatomic potentials in the 3D world, but the solutions for a few important models can be obtained analytically. These include the Percus-Yevick (PY) approximation [27, 28] for hard spheres and the mean spherical (MS) approximation for charged hard spheres, for hard spheres with point dipoles and for atoms interacting with a Yukawa potential. Numerical solutions for other approximations, such as the hypemetted chain (EfNC) approximation for charged systems, are readily obtained by fast Fourier transfonn methods... [Pg.478]

By using an effective, distance-dependent dielectric constant, the ability of bulk water to reduce electrostatic interactions can be mimicked without the presence of explicit solvent molecules. One disadvantage of aU vacuum simulations, corrected for shielding effects or not, is the fact that they cannot account for the ability of water molecules to form hydrogen bonds with charged and polar surface residues of a protein. As a result, adjacent polar side chains interact with each other and not with the solvent, thus introducing additional errors. [Pg.364]

Individual chains are planar with alternating cis—trans conformation along the chain, and the interaction with neighboring chains leads to a highly ordered matrix. [Pg.241]

Chemical Interaction. Halogens and some phosphoms flame retardants act by chemical interaction. The flame retardant dissociates into radical species that compete with chain propagating and branching steps in the combustion process. [Pg.465]

Viscosity Index Improvers. VI improvers are long-chain, high molecular weight polymers that increase the relative viscosity of an oil at high temperatures more than at low temperatures. In cold oil the molecules of the polymer adopt a compressed coiled form so that the affect on viscosity is minimized. In hot oil the molecules swell, and interaction with the oil produces a proportionally greater thickening effect. Although the viscosity of the oil—polymer mixture decreases as the temperature increases, viscosity does not decrease as much as the oil alone would decrease. [Pg.265]

Crystallinity of polypropylene is usually determined by x-ray diffraction (21). Isotactic polymer consists of heHcal molecules, with three monomer units pet chain unit, resulting in a spacing between units of identical conformation of 0.65 nm (Fig. 2a). These molecules interact with others, or different... [Pg.407]

A range of plasticizer molecule models and a model for PVC have been generated and energy minimized to observe their most stable conformations. Such models highlight the free volume iacrease caused by the mobiHty of the plasticizer alkyl chains. More detailed models have also been produced to concentrate on the polar region of the plasticizer and its possible mode of interaction with the polymer. These show the expected repulsion between areas on the polymer and plasticizer of like charge as weU as attraction between the negative portions of the plasticizer and positive portions of the PVC. [Pg.124]

Reasons for these trends are clearly related to the polarity of the plasticizer and its abiUty to impart free volume by chain separation. Differences in polarity affect the temperature at which the plasticizer can penetrate the polymer matrix and the magnitude of the interaction with the polymer chain that results. [Pg.126]

EIectrosta.tlcs. Electrostatic interactions, such as salt bridges, result from the electrostatic attraction that occurs between oppositely charged molecules. These usually involve a single cation, eg, the side chain of Lys or Arg, or the amino terminus, etc, interacting with a single anion, eg, the side chain of Glu or Asp, or the carboxyl terminus, etc. This attractive force is iaversely proportional to the distance between the charges and the dielectric constant of the solvent, as described by Coulomb s law. [Pg.196]

A Acylsarcosinates. Sodium A/-lautoylsarcosinate [7631-98-3] is a good soap-like surfactant. Table 4 gives trade names and properties. The amido group in the hydrophobe chain lessens the interaction with hardness ions. A/-Acylosarcosinates have been used in dentifrices (qv) where they ate claimed to inactivate enzymes that convert glucose to lactic acid in the mouth (57). They ate prepared from a fatty acid chloride and satcosine ... [Pg.238]

Metal carboxyiates have been considered as nucleophilic agents capable of removing aHyUc chlorine and thereby affording stabilization (143). Typical PVC stabilizers, eg, tin, lead, or cadmium esters, actually promote the degradation of VDC polymers. The metal cations in these compounds are much too acidic to be used with VDC polymers. An effective carboxylate stabilizer must contain a metal cation sufftcientiy acidic to interact with aHyUc chlorine and to facihtate its displacement by the carboxylate anion, but at the same time not acidic enough to strip chlorine from the polymer main chain (144). [Pg.438]

Anionic Surfactants. PVP also interacts with anionic detergents, another class of large anions (108). This interaction has generated considerable interest because addition of PVP results in the formation of micelles at lower concentration than the critical micelle concentration (CMC) of the free surfactant the mechanism is described as a "necklace" of hemimicelles along the polymer chain, the hemimicelles being surrounded to some extent with PVP (109). The effective lowering of the CMC increases the surfactant s apparent activity at interfaces. PVP will increase foaming of anionic surfactants for this reason. [Pg.532]


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See also in sourсe #XX -- [ Pg.372 ]

See also in sourсe #XX -- [ Pg.372 ]




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Chain interactions

Chains with two-body interactions real space expansions

Effective calculations isolated chain with two-body interaction

Effective calculations set of chains with two-body interactions

Elimination of short range divergences for a chain with two-body interactions

Interactions with neighboring chains

On a few simple properties of chains with repulsive interactions

Polynuclear chains with direct interactions between heavy atoms

Real Polymer Chains with Large Frictional Interactions

Recoil growth algorithm for chain molecules with continuous interactions

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