Journal of the Textile Machinery Society of Japan
Online ISSN : 1881-1159
Print ISSN : 0040-5043
Volume 26, Issue 2
Displaying 1-4 of 4 articles from this issue
  • Kiyoji Nakamura, Takuji Higashi, Akira Horikawa
    1980Volume 26Issue 2 Pages 35-41
    Published: 1980
    Released on J-STAGE: October 24, 2006
    JOURNAL FREE ACCESS
    The effect of inlet angles of a tapered channel on viscoelastic flows in a Maxwell model was numerically investigated by the perturbation method using oblique coordinates. These results have shown that the characteristic flow pattern of viscoelastic liquids such as a shape of a wine glass is produced by the sudden contraction into the slit rather than by turning round the corner, and, in addition, that the inlet angle of a tapered channel has little effect on the shape of the main flow.
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  • Part 2 Viscoelastic Body Composed of Broad Distribution of Relaxation Time
    Sei-ichi Manabe, Kenji Kamide, Chozo Nakayama
    1980Volume 26Issue 2 Pages 42-50
    Published: 1980
    Released on J-STAGE: October 24, 2006
    JOURNAL FREE ACCESS
    In order to establish the relationship between the distribution function Fτ(τ) of relaxation time τ and the shape and the characteristic parameters of dynamic loss tangent (tanΔ)-temperature (T) curves, theoretical equations representing tanΔ-T curves are derived; seven functions given by Fτ(τ)=knn' and three functions given by triangles. WLF and Arrhenius types are assumed for temperature dependence of τ. On the basis of these theoretical equations, tanΔ-T curves are numerically calculated. In the case of n'_??_0, the peak value of tanΔ-T curve, (tanΔ)max, peak temperature Tmax and the ratio of half value width ΔT1/2T1/2 (s) (the suffix s indicates the system composing of a single relaxation time) depend on those factors as the average relaxation time τ, Fτ, the total number of Maxwell elements in a system N, the ratio of elastic modulus before and after relaxation α, and the minimum relaxation time τl in Fτ(τ). In the case of n'_??_-0.5, a significant shoulder is observed on tanΔ-T curves in the lower temperature region than Tmax. The necessary condition to have this shoulder is (tanΔ)max_??_3.5/(n'+3)4 and N_??_√<10>, The tanΔ-T curve (especially, ΔT1/2T1/2 (s) ), measured in the temperature range in which appears the dynamic absorption arising from microbrownian movement of polymer segments in amorphous region of semi-crystalline polymers (αa), is remarkably different from that calculated by using the above mentioned functions for Fτ(τ). Contrary to this, tanΔ-T curves determined experimentally in the temperature range of αa absorption of amorphous polymers are in good agreement with those calculated by using n'=-2-0. In the actual experiment, no shoulder, is observed on tanΔ-T curves for both amorphous and semi-crystalline polymers.
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  • Akira Shinohara, Takaaki Musha
    1980Volume 26Issue 2 Pages 51-54
    Published: 1980
    Released on J-STAGE: October 24, 2006
    JOURNAL FREE ACCESS
    This paper outlines the way to measure the bending length of comparatively stiff fabrics by the Clark method, and presents the theoretical basis of this method. We derived the relation theoretically between the bending length and the hanging length of the specimen at the critical angle at which swing back occurs on the assumption that the test specimen is completely elastic. This theory is applicable to measure the bending length by the Clark Stiffness Tester, which correlates well to the 41.5° cantilever method. But the Clark method gives approximately 10% smaller values than the 41.5° cantilever method.
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  • Tsuneo Horino, Shinsuke Iwamoto
    1980Volume 26Issue 2 Pages 55-57
    Published: 1980
    Released on J-STAGE: October 24, 2006
    JOURNAL FREE ACCESS
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