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  • 1
    Electronic Resource
    Electronic Resource
    New York : Wiley-Blackwell
    Journal of Polymer Science Part A: General Papers 1 (1963), S. 2477-2486 
    ISSN: 0449-2951
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The orientation of flexible, coiled, chain macromolecules in the velocity field with parallel gradient has been analyzed on the basis of the subchain model. It has been found that the axial orientation factor in the steady state depends only on the velocity gradient q, diffusion constant D, and molecular dimensions. The internal viscosity of macromolecule has no influence upon the steady-state orientation factor. The relation describing the time dependence of the orientation factor have also been derived.
    Additional Material: 4 Ill.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    New York : Wiley-Blackwell
    Journal of Polymer Science Part A: General Papers 1 (1963), S. 2487-2494 
    ISSN: 0449-2951
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The intrinsic viscosity of dilute solutions containing flexible chain macromolecules flowing in a velocity field with parallel gradient has been analyzed. It has been found that the viscosity at rest is three times the value of the shearing viscosity. The viscosity increases monotonically with velocity gradient (steady flow) and with time (at constant gradient). On the basis of the results of this and previous papers, general features of the dynamic behavior of dilute polymer solutions flowing in the velocity field with parallel gradient have been discussed.
    Additional Material: 2 Ill.
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  • 3
    Electronic Resource
    Electronic Resource
    New York : Wiley-Blackwell
    Journal of Polymer Science Part A: General Papers 1 (1963), S. 507-515 
    ISSN: 0449-2951
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: On the basis of Jeffery's general relations, formulas for the rate of dissipation of energy due to the motion of a rigid rotational ellipsoid in a liquid, uniaxially drawn, were derived. By use of the previously found distribution function, intrinsic viscosity v, was calculated and effects of ellipsoid shape, velocity gradient, diffusion rate constant and time were discussed. The intrinsic viscosity monotonically increases with velocity gradient and with time t. This behavior is quite different from that observed in shear flow. It was stated that phenomena connected with a velocity field with parallel gradient (i.e., flow with uniaxial deformation): \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm V}_{ij} = \left( {\begin{array}{*{20}c} q & 0 & 0 \\ 0 & {{\rm - }\sigma q} & 0 \\ 0 & 0 & {{\rm - }\sigma q} \\ \end{array}} \right) $\end{document} such as liquid jets, fiber spinning etc., cannot be explained in terms of experiments or theories concerning the shear flow (velocity field with perpendicular gradient): \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm V}_{ij} = \left( {\begin{array}{*{20}c} 0 & q & 0 \\ q & 0 & 0 \\ 0 & 0 & 0 \\ \end{array}} \right) $\end{document} as obtained in viscosity measurements in common types of viscometers (capillary, rotational, falling body), or investigations of flow birefringence in coaxial apparatus.
    Additional Material: 4 Ill.
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  • 4
    Electronic Resource
    Electronic Resource
    New York : Wiley-Blackwell
    Journal of Polymer Science Part A: General Papers 1 (1963), S. 491-506 
    ISSN: 0449-2951
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: The spatial orientation of rigid ellipsoidal particles was analyzed as proceeding in a dilute solution flowing in a velocity field with parallel gradient, i.e., in a field characterized by the deformation rate tensor: \documentclass{article}\pagestyle{empty}\begin{document}$ {\rm V}_{ij} = \left( {\begin{array}{*{20}c} q & 0 & 0 \\ 0 & { - 1/2q} & 0 \\ 0 & 0 & { - 1/2q} \\ \end{array}} \right) $\end{document} On the basis of general relations given by Jeffery, the hydrodynamic equations of motion of a single ellipsoid were obtained as Ψ = 0, ϕ = 0, θ = -¾qR sin 2θ, where q = ∂Vκ/∂κ is the parallel velocity gradient and R = (a2 - b2)/(a2 + b2) is the shape coefficient of ellipsoids. Considering the action of velocity field and that of Brownian motion (rotational diffusion), a distribution density function ρ(t, θ) was derived, which describes the spatial orientation of the axes of symmetry of the ellipsoids: \documentclass{article}\pagestyle{empty}\begin{document}$ \rho (t,\theta ){\rm = }F_0 {\rm } - {\rm }[F_0 {\rm } - {\rm (1}/4\pi )]{\rm exp }\left\{ { - {\rm }\lambda _{1{\rm }} tD} \right\} $\end{document} where \documentclass{article}\pagestyle{empty}\begin{document}$ F_0 \left( \theta \right) = \left( {{1 \mathord{\left/ {\vphantom {1 {4\pi }}} \right. \kern-\nulldelimiterspace} {4\pi }}} \right)\left\{ {1{\rm } + {\rm }\left( {{{\alpha R} \mathord{\left/ {\vphantom {{\alpha R} 4}} \right. \kern-\nulldelimiterspace} 4}} \right)\left( {3\cos ^2 \theta {\rm } - {\rm }1} \right) + \left( {{9 \mathord{\left/ {\vphantom {9 4}} \right. \kern-\nulldelimiterspace} 4}} \right)\left( {\alpha R} \right)^2 \left[ {.{\rm }.{\rm }.} \right]{\rm } + {\rm }{\rm . }{\rm . }{\rm . }} \right\} $\end{document} is the steady-state distribution. In a similar way, the axial orientation factor f0 = 1 - 3/2 sin2θ was obtained: \documentclass{article}\pagestyle{empty}\begin{document}$ f_0 = \left( {{7 \mathord{\left/ {\vphantom {7 5}} \right. \kern-\nulldelimiterspace} 5}} \right)\left[ {\left( {{{\alpha R} \mathord{\left/ {\vphantom {{\alpha R} {14}}} \right. \kern-\nulldelimiterspace} {14}}} \right) + \left( {{{\alpha R} \mathord{\left/ {\vphantom {{\alpha R} {14}}} \right. \kern-\nulldelimiterspace} {14}}} \right)^2 - \left( {{7 \mathord{\left/ {\vphantom {7 5}} \right. \kern-\nulldelimiterspace} 5}} \right)\left( {{{\alpha R} \mathord{\left/ {\vphantom {{\alpha R} {14}}} \right. \kern-\nulldelimiterspace} {14}}} \right)^3 + \left( {{{\alpha R} \mathord{\left/ {\vphantom {{\alpha R} {14}}} \right. \kern-\nulldelimiterspace} {14}}} \right)^4 \left( {.{\rm }.{\rm }.} \right) + {\rm }{\rm . }{\rm . }{\rm .}} \right] $\end{document}
    Additional Material: 8 Ill.
    Type of Medium: Electronic Resource
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