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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 74 (1952), S. 1977-1979 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Chemical reviews 39 (1939), S. 79-135 
    ISSN: 1520-6890
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 57 (1935), S. 2347-2351 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [s.l.] : Nature Publishing Group
    Nature 191 (1961), S. 1160-1161 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] IN a recent paper1 we directed attention to the fact that values of both intrinsic viscosity [YJ] and the viscosity slope constant Jc', obtained in the usual way, may be significantly in error because of an apparent reduction in capillary radius. As Ohm2 has demonstrated, this apparent reduction in ...
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [s.l.] : Nature Publishing Group
    Nature 196 (1962), S. 1197-1198 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] (a) The third paragraph of the earlier communication should be replaced by the following: From this it follows that, in sufficiently dilute solutions: spC (2) and for in such solutions: ktfr = In (1 + tsp) = (3) Subtracting (3) from (2), we obtain: - - -- = -5- hn] 4- (TT -f k' ' -n c c R L ...
    Type of Medium: Electronic Resource
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  • 6
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The viscosity slope constant k′, i.e., \documentclass{article}\pagestyle{empty}\begin{document}$ \mathop {\lim }\limits_{c \to 0} \frac{{d\left( {{{\eta _{sp} } \mathord{\left/ {\vphantom {{\eta _{sp} } c}} \right. \kern-\nulldelimiterspace} c}} \right)}}{{dc}}\frac{1}{{[\eta ]^2 }} $\end{document}, is shown to be of increasing significance in polymer science as a molecular-weight-independent criterion of solvent power and as a parameter sensitive to various changes in polymer structure, such as long-chain branching. Ideally, it is a dimensionless parameter, independent of molecular size, which arises only from the mutual hydrodynamic interaction of polymer molecules and depends, therefore, on the intrinsic flexibility of the polymer chain and on the polymer density in the coiled molecule. In real systems, however, other interactions may contribute, sometimes very significantly, to k′. For such real systems, the general expression: \documentclass{article}\pagestyle{empty}\begin{document}$ k' = k + a + \frac{K}{{[\eta ]^2 }}\left( {[\eta ]_{(2)} - [\eta ]_{(1)} } \right) $\end{document} is suggested. In ternary systems, polymer-polymer-solvent, ideal expressions for ηsp/c and k′ are developed, that for k′ being: \documentclass{article}\pagestyle{empty}\begin{document}$ k' = \sum\limits_i {\sum\limits_j {\surd \bar k_i [\eta ]_i w_i {{\surd \bar k_j [\eta ]_i w_i } \mathord{\left/ {\vphantom {{\surd \bar k_j [\eta ]_i w_i } {(\sum\limits_i {[\eta ]_i w_i } )^2 }}} \right. \kern-\nulldelimiterspace} {(\sum\limits_i {[\eta ]_i w_i } )^2 }}} } $\end{document} It is proposed that deviations from ideal behavior so defined are due to nonhydrodynamic polymer-polymer interactions and might be used to detect and measure the strength of such interactions. Some preliminary data for the system polystyrene-poly(methyl methacrylate)-m-xylene are presented and discussed.
    Additional Material: 3 Ill.
    Type of Medium: Electronic Resource
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  • 7
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The viscosity behavior of a high molecular weight fraction (M̄w = 9.8 × 106) of dextran (B-512) in aqueous solutions was studied at low and medium shear stresses, and its intrinsic viscosity was shown to be independent of shear stress. A convenient and precise multibulb Ubbelohde-type viscometer, especially designed for use with aqueous solutions is described. The calibration of the viscometer and the evaluation of surfacetension corrections of relative flow times measured in it are discussed in detail.
    Additional Material: 3 Ill.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 13 (1954), S. 167-174 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: For the viscometric determination of the molecular weight of a flexible linear high polymer, a very “poor” solvent in which the osmotic slope constant B is zero (i.e., a so-called “ideal” solvent) has several advantages over the usually preferred good ones. For example, shear effects that are very troublesome with very high polymers in good solvents become negligible or easily manageable. Moreover, in an “ideal” solvent, the “contents” K and a in the equation relating [η] and M really are constant over a very wide range of molecular weights and, since a always has the value 0.50, are more easily determined. Because the advantages seem to outweigh considerably the disadvantages, the use of an “ideal” solvent should be given careful consideration, particularly when the molecular weights are very high or cover a wide range.
    Additional Material: 2 Ill.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 32 (1958), S. 187-192 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: Evidence of a critical concentration effect in dilute polymer solution has been obtained from light-scattering measurements in two ternary systems of the type polymer A-polymer B-solvent S. The root-mean-square end-to-end distance, (r2)1/2, of A was measured in a series of mixed solvents (B-S), differing from one another only in respect Of CB, the concentration of polymer B. The (r2)1/2 vs. CB curve exhibited a slight dip in the system polystyrene-polyvinyl acetate-benzene and a slight peak in the system polystyrene-polyvinyl acetate-butanone, at values of CB close to but not identical with the critical concentrations determined viscometrically for the same systems. The size, nature, and location of these light-scattering critical concentration effects are briefly discussed in the light of similar but better established viscosity effects.
    Additional Material: 1 Ill.
    Type of Medium: Electronic Resource
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  • 10
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: Measurements of intrinsic viscosity and light scattering were made on fractions of polymers prepared by the redox polymerization of styrene in the presence of oxidized polystyrene or copolymers of skyrene and 4-vinylcyclohexene-1. For comparison, similar measurements were made on fractions of linear polystyrene. The conclusion that branching had taken place by graft polymerization was confirmed. Values found for the intrinsic viscosity, the molecular size, and the second virial coefficient were generally lower for fractions of the graft polymers than for fractions of linear polystyrene of the same molecular weight. It was also observed that fractionation of the graft polymers took place with respect to molecular size, not molecular weight, and that the most highly branched fractions were the most soluble. A comparison of experimental values of the branching ratio g with values calculated for a model having linear branches equally spaced along a backbone chain indicates that the graft polymers contain up to at least 6 branches per molecule. Values of Huggins' k′ for these branched molecules did not differ significantly from those for linear polystyrene (0.30 〈 k′ 〈 0.40). It is concluded that though k′ is sensitive to bushy branching, it is not measurably affected by the presence in the polymers of a few linear branches per molecule.
    Additional Material: 4 Ill.
    Type of Medium: Electronic Resource
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