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  • 1
    Electronic Resource
    Electronic Resource
    Bognor Regis [u.a.] : Wiley-Blackwell
    Journal of Polymer Science Part B: Polymer Physics 27 (1989), S. 819-835 
    ISSN: 0887-6266
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The rheological behavior of the thermotropic liquid crystal copolyesters composed of p-hydroxybenzoic acid and 2-hydroxy-6-naphthoic acid (indicated as HBA/HNA) is investigated for three different compositions: 75:25, 58:42, 30:70 (in mol%). The inherent viscosities are 9.2, 5.1, and 7.8 dl/g, respectively. Yield stress is observed for all three samples. This indicates the existence of crystallites in the melt which may be related to the shear thinning viscosity at low shear stress. Melt fracture, and a die swell ratio which increases with shear rate, are also observed at higher temperatures and at low shear stress for the two copolyesters having compositions 75:25 and 30:70. We have also estimated for 30HBA/70HNA at 335°C the entrance pressure loss, Δpent, and ΔPent/δw, where δw is the shear stress at the capillary wall. The large value of ΔPent/δw suggest that HBA/HNA is a highly elastic polymeric material. It is found that both ΔPent and ΔPent/δw increase with shear rate. However, the high elasticity does not account for the disappearance of melt fracture and contraction of die swell at high shear stress. This abnormal phenomenon is ascribed to the formation of a network of crystallites caused by blocky regions in the copolymer.
    Additional Material: 18 Ill.
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  • 2
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: In applying the quadratic form π/c = (π/c)0[1 + Γ2c + Γ3c2] to osmotic pressure of dilute polymer solutions, the use of a third coefficient (Γ3), which is related semitheoreti-cally to the second (Γ2), is to be recommended over the use of unrestricted coefficients, both from the standpoint of expediency and of accuracy in the values so obtained for the intercept (π/c)0. and the initial slope (π/c)0Γ2.
    Additional Material: 1 Ill.
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  • 3
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: Intrinsic viscosities of low molecular weight polystyrene fractions measured in an “ideal” solvent (i.e., in cyclohexane at the “θ temperature,” 34°C.) are in accord with the relationship [η]θ = KM1/2. Even at a molecular weight of only 4000, the observed value of K agrees with that for high molecular weights.
    Additional Material: 1 Ill.
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  • 4
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The lattice model treatment of athermal mixtures is reexamined by considering a two step process in which a growing chain forms an interference with a completed molecule. The expectancy, f, that an interference will arise is given by the product of the respective probabilities, P, and Q, that each step will occur. For low solute concentrations, the result is nearly the same as a revised form of the equation derived in various ways by Huggins, Miller, Orr, and Guggenheim. The same result is obtained for linear, bent, or branched molecules, but only so long as no ring-forming intramolecular contacts exist. Dilute solutions of coiling polymer molecules require special treatment, due to a variable number of intramolecular 2-2 contacts that depends upon the average molecular configuration. Branching, through its effect on molecular configuration, will after the dilute solution properties. The effect of branching and intramolecular contacts should become less important as the polymer concentration is increased. As the volume fraction of solute is increased, both of the probabilities, P and Q, become rapidly varying functions of this variable. An approximate calculation based on the two-step encounter process yields values for f nearly equal to the average expectancy f̄ that a randomly selected site will be occupied. The latter was empolyed in the treatment of Flory. Thus, the refinements introduced by Huggins and others are only applicable to dilute solutions of noncoiling molecules. This furnishes an explanation for the observation that the proposed refinements do not improve the agreement with experiment shown by the simpler expression due to Flory.
    Additional Material: 4 Ill.
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  • 5
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 33 (1958), S. 532-533 
    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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  • 6
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 33 (1958), S. 533-534 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    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: Intrinsic viscosities of polystyrene and polyisobutylene fractions in good and in “ideal” solvents have been examined from the point of view of their dependence on molecular weight. A compilation of results is presented which covers exceptionally wide ranges, from several thousand to several to million, in molecular weight. The intrinsic viscosity in an “ideal” solvent (i.e., cyclohexane at 34°C. for polystyrene, or benzene at 24° for polyisobutylene) is remarkably well fitted over the molecular weight range cited above by the relation: \documentclass{article}\pagestyle{empty}\begin{document}$$ [\eta]\Theta = KM^{1/2} $$\end{document} where K is a constant, independent of molecular weight, for a particular polymer at a given temperature. The molecular expansion factor α3 which applies in good solvents (e.g., toluene for polystyrene and cyclohexane and diisobutylene for polyisobutylene) as calculated from: \documentclass{article}\pagestyle{empty}\begin{document}$$ [\eta] = KM^{1/2} \alpha^3 $$\end{document} increases with molecular weight approximately in accordance with the relationship: \documentclass{article}\pagestyle{empty}\begin{document}$$ \alpha^5 - \alpha^3 = 2C_{M\psi 1} (1 - \Theta /T)M^{1/2} $$\end{document} However, the quantity (α5 - α3)/M1/2 changes appreciably with M in some cases. This is particularly true for molecular weights below 50,000. Results of an examination of the effect of rate of shear on the viscosity of polystyrene in benzene at 25° and in cyclohexane at 34°, and of the intrinsic viscosity-molecular weight relation for polystyrene in benzene at 25°, are reported.
    Additional Material: 7 Ill.
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  • 8
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 18 (1955), S. 107-121 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: A recent treatment of phase equilibria in nonpolar ternary systems is modified to permit application to the interesting case of a polymer and two polar liquids which may associate. The deviations from ideality exhibited by associated liquids are incorporated with the pair interaction free energy in the X parameter for the liquid pair. Hence, the expressions for the chemical potentials remain unaltered, but the X parameters for the polar liquid pair are concentration dependent; furthermore, the relation X12 = (V1/V2)X21, no longer applies. The equation deduced allows theoretical description of the phase equilibria in polar ternary systems provided sufficient information is available to characterize the binary polar liquid mixture. The predictions arising from the modified theory are tested using data obtained from phase composition analysis of the two ternary systems: nitrocellulose-ethanol-water and nitrocellulose-diethylene glycol-water. The isotherms obtained for the former system provide excellent confirmation of the theoretical predictions. Although for the second system studied the polymer-solvent interaction parameters appear to be concentration dependent; nevertheless, application of theory yields values for the difference (lX′23 - X′13) over the concentration range of interest. The (lX′23 - X′13) differences deduced from the data for both ternary systems yield values for the nitrocellulose-water interaction parameter which stand in good agreement with the value directly deduced from the sorption isotherm for that binary system, thus providing further confirmation of the theoretical treatment.
    Additional Material: 7 Ill.
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  • 9
    Electronic Resource
    Electronic Resource
    Hoboken, NJ : Wiley-Blackwell
    Journal of Polymer Science 28 (1958), S. 213-221 
    ISSN: 0022-3832
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: A procedure is described for estimating unperturbed molecular dimensions from data obtained in “nonideal” solvents. A knowledge of [η], M, and A2 is required. This should be particularly useful for high melting crystalline polymers, since for these polymers a direct determination by light scattering measurements performed under Flory θ conditions is complicated by the tendency of the polymer to crystallize from solution as the solvent becomes thermodynamically poorer. The intrinsic viscosity at θ, [η]θ, is calculated from the semi-empirical relation: \documentclass{article}\pagestyle{empty}\begin{document}$$ [\eta ] - [\eta ]_\theta = 5 \times 10^{ - 3} \Gamma _2 $$\end{document} where Γ2 = A2M. The unperturbed dimensions are then calculated through use of the relations appearing in Flory's treatment of intrinsic viscosity: \documentclass{article}\pagestyle{empty}\begin{document}$$ \begin{array}{*{20}c} {[\eta ]_\theta = KM^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 2}}\right.\kern-\nulldelimiterspace} \!\lower0.7ex\hbox{$2$}}} } & {{\rm and}} & {\left( {{{\overline {L_0^2 } } \mathord{\left/ {\vphantom {{\overline {L_0^2 } } M}} \right. \kern-\nulldelimiterspace} M}} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 2}}\right.\kern-\nulldelimiterspace} \!\lower0.7ex\hbox{$2$}}} = \left( {{K \mathord{\left/ {\vphantom {K \Phi }} \right. \kern-\nulldelimiterspace} \Phi }} \right)^{{\raise0.7ex\hbox{$1$} \!\mathord{\left/ {\vphantom {1 3}}\right.\kern-\nulldelimiterspace} \!\lower0.7ex\hbox{$3$}}} } \\ \end{array} $$\end{document}Unperturbed dimensions calculated in this manner for polyisobutylene and polystyrene compare favorably with values directly measured by light scattering. This procedure is used to estimate the unperturbed dimensions of polyethylene, 6,6-nylon, polyethylene terephthalate, and polyacrylonitrile. A comparison of the relative chain stiffness of these polymers allows some interesting correlations with Flory's theoretical treatment of semi-flexible chain molecules.
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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: Mixtures of fractions of atactic polystyrene dissolved in cyclohexane were resolved by elution from a column at different temperatures. A coarse-grained Ottawa sand was used to minimize the surface area of the support. Comparison with the critical miscibility temperature data of Schultz and Flory shows that the lower molecular weights are eluted from the column at a temperature somewhat below the critical miscibility temperature, as expected, but for molecular weights above 3 × 105 the elution temperature increases abruptly, and even exceeds the critical miscibility temperature. This rapid rise occurred at 1.5 × 105 when the surface area of the support was increased by use of a very fine Celite. We conclude that for the higher molecular weights additional thermal energy is required to desorb the polymer, and hence the partitioning of these species is not determined solely by solubility considerations. Concerning the efficiency of the column extraction, considerable resolution of each component was obtained, and attempts to determine the M̄w/M̄n ratios of the individual components were at least partially successful. As predicted by theory, for a given molecular weight interval the range of elution temperature was increased fivefold by the use of a mixed solvent, benzene-ethanol, in place of the single poor solvent, cyclohexane. Customary fractionation procedures are very inefficient when applied to high-melting crystalline polymers. For these polymers we investigated selective precipitation upon a column having a temperature gradient, rather than elution from the column. For dilute solutions, amorphous phase separation may precede crystallization, particularly in the case of polymers whose rates of crystallization are low, owing to the presence of bulky side groups. The column precipitation method failed to give improved fractionation of polyacrylonitrile, owing to phase separation of the dimethylformamide-heptane mixture part way down the column. On the other hand, good resolution was obtained for an unfractionated sample of isotactic polystyrene up to 1.5 × 106. Molecular weights above this level were compressed into a narrow band at the top of the column. Thus, if the distribution is extremely broad, a second fractionation with a different solvent:- precipitant ratio may be required. Even so, a single pass through the column resulted in a better resolution than that obtained by a large-scale, two-stage extraction-precipitation procedure, indicating that the column precipitation method does posses an advantage for the fractionation of crystalline polymers.
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