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  • Polymer and Materials Science  (268)
  • Wiley-Blackwell  (268)
  • American Geophysical Union
  • Institute of Physics
  • 1955-1959  (268)
Collection
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  • Wiley-Blackwell  (268)
  • American Geophysical Union
  • Institute of Physics
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Year
  • 1
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The dilute solution viscosity properties of fractions of two linear and one branched sample of polyvinyl acetate in benzene and of two linear and one branched fraction in several solvents were measured at 35°C. Values of total slope, b (from plots of ηsp/c vs. c), and intrinsic viscosities were obtained under the requirement that k′ + β = 0.500 ± 0.002. Empirical plots of log b vs. log [η] gave lines which were straight within the limits of accuracy of the data. For the linear fractions in benzene, Huggins' k′ was constant and the slope of the log b vs. log [η] line was 2; for the branched fractions in benzene, k′ increased with [η] and the slope of the log b vs. log [η] line was greater than 2. The log b vs. log [η] plots form the basis for a “one-point” method for determining [η]. Consideration of these data along with results reported in the literature indicates that k′ is measurably sensitive to branching only for fractions possessing a certain minimum combination of size and complexity. However, in some cases where the variations of k′ are inconclusive, use of the slope of the log b vs. log [η] line may provide a reliable indication of branching. It was found that a comparison between the branched and linear series could also be made at constant values of [η] or b. Two linear fractions in different solvents obeyed a type of Huggins relationship in which k′ did not vary with solvent and the slope of the log b vs. log [η] line was 2. For a higher molecular weight branched fraction, however, k′ varied from solvent to solvent and the slope of the log-log plot was about 1.7. These data do not support a reference point concept of “true” intrinsic viscosity based on a simple linear relationship between b and [η]. Preliminary results dealing with the effects of the shear rate indicated that the measured viscosity properties of branched fractions may be more seriously affected by changes in shear rate than those of linear fractions.
    Additional Material: 5 Ill.
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  • 2
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 40 (1959), S. 457-468 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: New equations for evaluation of resonance (q) and electrical (∊) factors affecting copolymerization have been derived: \documentclass{article}\pagestyle{empty}\begin{document}$ \begin{array}{*{20}c} {r_1 } \hfill & { = \exp \left\{ { - {{\left( {q_1 - q_2 } \right)} \mathord{\left/ {\vphantom {{\left( {q_1 - q_2 } \right)} {RT}}} \right. \kern-\nulldelimiterspace} {RT}}} \right\}\exp \left\{ { - 7.23 \times 10^{20} \varepsilon _1 {{\left( {\varepsilon _1 - \varepsilon _2 } \right)} \mathord{\left/ {\vphantom {{\left( {\varepsilon _1 - \varepsilon _2 } \right)} {RT}}} \right. \kern-\nulldelimiterspace} {RT}}} \right\}} \hfill \\ {r_2 } \hfill & { = \exp \left\{ { - {{\left( {q_2 - q_1 } \right)} \mathord{\left/ {\vphantom {{\left( {q_2 - q_1 } \right)} {RT}}} \right. \kern-\nulldelimiterspace} {RT}}} \right\}\exp \left\{ { - 7.23 \times 10^{20} \varepsilon _2 {{\left( {\varepsilon _2 - \varepsilon _1 } \right)} \mathord{\left/ {\vphantom {{\left( {\varepsilon _2 - \varepsilon _1 } \right)} {RT}}} \right. \kern-\nulldelimiterspace} {RT}}} \right\}} \hfill \\ {r_1 r_2 } \hfill & { = \exp \left\{ { - 7.23 \times 10^{20} {{\left( {\varepsilon _1 - \varepsilon _2 } \right)^2 } \mathord{\left/ {\vphantom {{\left( {\varepsilon _1 - \varepsilon _2 } \right)^2 } {RT}}} \right. \kern-\nulldelimiterspace} {RT}}} \right\}} \hfill \\ \end{array} $\end{document} The new equations will apply over any temperature range, and will express ∊ in terms of e.s.u. and q in kcal./mole. These factors were determined for an extensive list of monomers and were tabulated. Agreement with Hammett σ values and other kinetic and theoretical considerations were found.
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  • 3
    ISSN: 0021-8995
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: A number of fluorinated polyesters have been prepared by condensing hexafluoropentanediol with one or more dibasic acid chlorides, and melting and glass transition temperatures and rates of crystallization have been determined, largely by means of volume dilatometry. The relation between [η] in chloroform at 30° and M̄n for hexafluoropentylene adipate (HFPA) was found to be [η] = 3.20 × 10-5 M̄n. The melting point Tm was found to increase from 34.5° to 104° as the isophthalate content in a series of adipate copolyesters increased from 0 to 100 mole-%. The glass transition Tg increases from -57° to -31° as isophthalate content increases from 0 to 50 mole-%. Tg is raised about 6° by the crosslinking of the polyesters. Rates of crystallization were determined for two HFPA samples with M̄n's of 13,000 and 19,500. Maxima in these rates occurred at about -13° and -15°, respectively. Respective t½ values for (linear) HFPA, vulcanized HFPA, and a copolyester containing 20 mole-% isophthalate are 48, 1140, and 27,200 min., respectively, at -10°. All the crystallization isotherms conform to Avrami's equation, (Vt - V∞)/(Vt - V∞) = exp {-αt″} for n = 6 over the initial stages of the process. At 1° both HFPA isotherms agree with the above equation over a large part of the process; however, as the isotherm temperature decreases, the equilibrium degree of crystallinity, as judged by the overall specific volume change, decreases and the isotherms diverge from Avrami's equation over progressively larger portions of the process. The product of the maximum rate of crystallization for each isotherm with either t½ or τi, the “induction time,” decreases with decreasing temperature, as would be expected in view of Avrami's equation. The value of 6 observed for n, a constant determined by the nucleation and growth mechanisms, is anomalous since only values of 1 to 4 are theoretically predictable. Values over the range of 1 to 4 have been observed experimentally by other workers for a variety of polymers.
    Additional Material: 7 Ill.
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  • 4
    Electronic Resource
    Electronic Resource
    New York, NY [u.a.] : Wiley-Blackwell
    Journal of Applied Polymer Science 1 (1959), S. 372-373 
    ISSN: 0021-8995
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Additional Material: 1 Ill.
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  • 5
    Electronic Resource
    Electronic Resource
    New York, NY [u.a.] : Wiley-Blackwell
    Journal of Applied Polymer Science 2 (1959), S. 358-362 
    ISSN: 0021-8995
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Polystyrene has been partially or completely modified to contain varying amounts of vinyl-trans-benzalacetophenone units in the polymer chain. Acetylation of polystyrene gave a pure poly(vinylacetophenone) which, when condensed with benzaldehyde, produced varying proportions of vinyl-trans-benzalacetophenone in the polymer. These styryl ketone polymers are very sensitive to ultraviolet radiation, thin layers becoming insoluble on brief exposure, yet can be stored in the dark for years without change.
    Additional Material: 4 Ill.
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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.
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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 capacity of cells containing solutions of 5% cellulose acetate in dioxane was measured from 50 cycles to as high as 5 megacycles by a bridge method. A dispersion region was found between zero and approximately 40 kc. The frequency where the dielectric dispersion was 0.50 was taken as the critical frequency which was found to be related to the viscosity determined degree of polymerization. An empirical correlation enabled the calculation of degrees of polymerization from dielectric dispersion which could be readily duplicated and which agreed reasonably well with those found by the viscosity method. It is suggested that this procedure may develop into a very convenient and rapid method for molecular weights pending the accumulation of further experimental evidence.
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  • 8
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 28 (1958), S. 453-454 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Additional Material: 1 Ill.
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  • 9
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 31 (1958), S. 235-237 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
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  • 10
    Electronic Resource
    Electronic Resource
    New York : Wiley-Blackwell
    Die Makromolekulare Chemie 20 (1956), S. 46-56 
    ISSN: 0025-116X
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Description / Table of Contents: Die Änderungen in der UR-Absorption von Kautschuk nach Cyklisierung werden beschrieben. Die Spektren von cyklisiertem Kautschuk, der bei Einwirkung von Schwefelsäure auf stabilisierten Hevea Milchsaft dargestellt wurde, zeigen, daß Cyklisierung auch bei Zimmertemperatur stattfindet. Die Spektraländerungen werden noch deutlicher wenn die Reaktion bei 80°C durchgeführt wird. Ein Vergleich der Spektren von cyklisiertem Kautschuk und 1,2-Dimethyl-Cyclohexen-1 deutet an, daß der cyklisierte Kautschuk substituierte Cyclohexen-Ring-Systeme enthält. Eine Absorption bei 13,17 μ war charakteristisch für cyclisierten Kautschuk.Die Änderungen in den UR-Absorption-Spektren von cyklisiertem Kautschuk nach Chloraddition werden ebenfalls diskutiert. Cyklisierter Kautschuk zeigt nach Chlorierung charakteristische Absorption von beiden, chloriertem und cyklisiertem Kautschuk.
    Notes: The changes in the infra-red absorption spectra of rubber following cyclization are reported. The spectra of cyclized rubber prepared by the action of sulphuric acid on stabilized Hevea latex have shown that cyclization starts even at room temperature. The spectral changes were more pronounced when the reaction was carried out at 80°C. From a comparison of the spectra of cyclized rubber with that of 1,2-dimethyl-cyclohex-1-ene, it is inferred that cyclized rubber contain substituted cyclohexene type rings. Absorption at 13.17 μ appeared to be characteristic of cyclized rubber.The changes in the infra-red absorption spectra of cyclized rubber, following additive chlorination are also discussed. Chlorinated cyclized rubber showed absorptions, characteristic of cyclized rubber and chlorinated rubber.
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