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Polymers molecular configuration

The treated phenomena and investigations summarized above are at the centre of the topic of this special two-volume edition of the Advances in Polymer Science on Intrinsic molecular mobility and toughness of polymers . However, little has been said about the mutual relations between molecular configuration, polymer morphology, nature, intensity and cooperativity of sub-Tg relaxation mechanisms, and mode of solicitation on the one hand and their effect on disentanglement, craze formation, yield behaviour and ultimate strength on the other. These subjects will be critically evaluated in the subsequent presentations of this Volume. [Pg.31]

A great many polymers appear to form films having a flat molecular configuration. Thus various polyesters [7] gave extrapolated areas of about 2.5 m /mg corresponding to about the calculated 60-70 area per segment, or mono-layer Sickness of 3-5 A. A similar behavior was noted for poly(vinyl acetate)... [Pg.539]

Gouinlock E. V., Flory P.J., Scheraga H.A.. Molecular configuration of gelatin. Journal of Polymer Science 16 (1955) 383-395. [Pg.112]

It may be shown that when the polymer concentration is large, the perturbation tends to be less. In particular, in a bulk polymer containing no diluent a = l for the molecules of the polymer. Thus the distortion of the molecular configuration by intramolecular interactions is a problem which is of concern primarily in dilute solutions. In the treatment of rubber elasticity—predominantly a bulk polymer problem—given in the following chapter, therefore, the subscripts may be omitted without ambiguity. [Pg.426]

In the present chapter we shall be concerned with quantitative treatment of the swelling action of the solvent on the polymer molecule in infinitely dilute solution, and in particular with the factor a by which the linear dimensions of the molecule are altered as a consequence thereof. The frictional characteristics of polymer molecules in dilute solution, as manifested in solution viscosities, sedimentation velocities, and diffusion rates, depend directly on the size of the molecular domain. Hence these properties are intimately related to the molecular configuration, including the factor a. It is for this reason that treatment of intramolecular thermodynamic interaction has been reserved for the present chapter, where it may be presented in conjunction with the discussion of intrinsic viscosity and related subjects. [Pg.596]

In order to understand polymer solution behaviour, the samples have to be characterised with respect to their molecular configuration, their molar mass and polydispersity, the polymer concentration and the shear rate. Classical techniques of polymer characterisation (light scattering, viscometry, ultracentrifugation, etc.) yield information on the solution structure and conformation of single macromolecules, as well as on the thermodynamic interactions with the solvent. In technical concentrations the behaviour of the dissolved polymer is more complicated because additional intramolecular and intermolecular interactions between polymer segments appear. [Pg.8]

There is no such thing as a pure polymer. All polymers comprise molecules that exhibit chemical and physical distributions of many variables these include molecular weight, branching, steric defects, molecular configuration, preferential chain orientation, and crystallite size and shape. The properties and characteristics that we exploit in polymers are controlled by the overall balance of these distributions. [Pg.31]

Flory,P. Molecular configuration in bulk polymers. Pure Appl. Chem. (in press). [Pg.165]

Rochefort S, Middleman S (1985) Effect of molecular configuration of xanthan gum drag reduction in Polymer-Flow Interaction ed Rabin Y, AIP Conf Proc 137 117... [Pg.164]

HDPE is a semi crystalline plastic, whose crystallinity varies from 40 to 80%. depending on the degree of branching and molecular weight. Polymer chains in crystalline HDPE have a flat zigzag configuration. The principal crystalline form of HDPE is orthorhombic, with a density of 1.00 g/cm3 and the cell parameters a =0.740, b = 0.493. and c ... [Pg.1142]

Fig. 4.5 Chromatogram representing print molecule (oxacillin) and two other /3-lactam antibiotics (penicillin G and V) on oxacillin MIP (a) compared with the control blank MIP (b). Reprinted from J. Chromatogr. A, 889, Briiggemann et al. New configurations and applications of molecularly imprinted polymers , 15-24 (2000), with permission... Fig. 4.5 Chromatogram representing print molecule (oxacillin) and two other /3-lactam antibiotics (penicillin G and V) on oxacillin MIP (a) compared with the control blank MIP (b). Reprinted from J. Chromatogr. A, 889, Briiggemann et al. New configurations and applications of molecularly imprinted polymers , 15-24 (2000), with permission...
It is perhaps obvious that the nature of the interface between a molecular solid (polymer) and a (clean) metal surface is not necessarily equivalent to the interface formed when a metal is vapor-deposited (essentially atom-by-atom ) on to the (clean) surface of the polymer or molecular solid. Atoms of all metals are active in the form of individual atoms , even gold atoms. In the context of the new polymer LEDs, some of the works discussed in chapter 7 involve the study of the early stages of formation of the interface in the latter configuration (metal-on-polymer interfaces). Very little has been reported on conjugated polymer-on-metal interfaces, however, primarily because of the difficulties in preparing monolayers of polymer materials on well defined metal substrates appropriate for study (via PES or any other surface sensitive spectroscopy). The issues discussed below are based upon information accumulated over two decades of involvement with the surfaces of condensed molecular solids and conjugated polymers in ultra-thin form, represented by the examples in the previous chapter. [Pg.140]

Doty, P., Wada, A., Yang, J. T., and Blout, E. R. (1957). Polypeptides VII. Molecular configurations of poly-L-glutamic acid in water-dioxane solution./. Polym. Sci. 23 851-861. [Pg.199]

Rich, A. Molecular configuration of synthetic and biological polymers. In Biophysical science, pp. 50—60, edited by J. L. Oncley. New York John Wiley Sons, Inc. 1959. [Pg.303]

Figure 16-9. Snapshots of molecular configurations for the solvated electron polymer at two supercritical densities of water at 645 K. Left 1.0 g/cm3 Right. 0.05 g/cm3... Figure 16-9. Snapshots of molecular configurations for the solvated electron polymer at two supercritical densities of water at 645 K. Left 1.0 g/cm3 Right. 0.05 g/cm3...

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See also in sourсe #XX -- [ Pg.559 , Pg.560 , Pg.561 ]




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