Sen'i Kikai Gakkaishi (Journal of the Textile Machinery Society of Japan)
Online ISSN : 1880-1994
Print ISSN : 0371-0580
ISSN-L : 0371-0580
Volume 31, Issue 1
Displaying 1-8 of 8 articles from this issue
  • Kenji Kamide, Sei-ichi Manabe, Masakatsu Hara, Chozo Nakayama
    1978 Volume 31 Issue 1 Pages T1-T10
    Published: January 25, 1978
    Released on J-STAGE: October 27, 2009
    JOURNAL FREE ACCESS
    By using the method proposed in the previous papers, the detailed fine structure in amorphous region of nylon 66 film and filament is disclosed from their dynamic loss tangent (tan δ) -temperature (T) curve. In annealing process, the elastic modulus fraction fe decreases and heterogeneity index of amorphous region nt increases monotonously with an increase in annealing temperature Ta for the unoriented film. In the annealing process of wet state, the fe related to α2 absorption, observed at 30°C (for 110 Hz), decreases more abruptly than that of α1 absorption observed at 120°C (for 110 Hz). On the contrary, in the annealing process of dry state, the fe related to α1 decreases more abruptly than α2. With an increase in stretching ratio, the fe of the stretched film and filament decrease and their nt increase monotonously. These tendencies of fe and nt during annealing and stretching are not limited to nylon 66, but have a general characters for another fiber-forming polymers, such as polyacrylonitrile, polyethyleneterephthalate, polypropylene and polyvinylalcohol.
    Both fe and nt-Ta curves of the stretched film show minimum when the film is annealed in dry state for a fixed time of period and nt increases nonotonously with Ta when the film is annealed in wet state. The complicated Ta dependence of fe and nt can be explained in termsof disorientation of oriented polymeric chains in the annealing process.
    A new peak in tan δ-T curve is observed at ca. 90°C (for 110 Hz) for the samples annealed in dry state at Ta=200°C. This peak is closely connected to the amorphous state produced during the annealing process. Several peaks are observed in the main dispersion region oftan δ-T curve, corresponding to the annealing in dry or wet state and adsorption of water and these can reasonably be resolved by the theory in the view of heterogenieties of the packing states of polymeric chains in amorphous region.
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  • K. Watanabe
    1978 Volume 31 Issue 1 Pages P3-P17
    Published: January 25, 1978
    Released on J-STAGE: October 27, 2009
    JOURNAL FREE ACCESS
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  • Part 1 : Method of Color Recognition
    Hitoshi Akami
    1978 Volume 31 Issue 1 Pages T11-T17
    Published: January 25, 1978
    Released on J-STAGE: October 27, 2009
    JOURNAL FREE ACCESS
    A color analyzer was developed which was completely different from conventional one using R, G and B optical filters. The process of color separation of the analyzer is carried out by the spectral pattern recognition.
    When 100 colors with 40% variance were recognized, the average rate of recognition of more than 99% was obtained. Therefore, this analyzer seems to be more useful than conventional procedures.
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  • Systems Design and Modeling
    H. Noshi, S. Uchiyama, M. Nakajima
    1978 Volume 31 Issue 1 Pages P18-P24
    Published: January 25, 1978
    Released on J-STAGE: October 27, 2009
    JOURNAL FREE ACCESS
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  • Part 3 : Theoretical Analysis of the Effective Heat Conductivity of Fiber Assembly
    Hirohito Matsui, Kazuo Moriyama
    1978 Volume 31 Issue 1 Pages T18-T27
    Published: January 25, 1978
    Released on J-STAGE: June 17, 2010
    JOURNAL FREE ACCESS
    A coefficient of effective diffusion is required to analyze the washing process of fiber assembly e.g., yarn, fabric, etc. The coefficient of effective diffusion has been estimated by analyzing theoretically the heat transmission under steady state within fiber assembly, and its effective heat conductivity was calculated.
    The effective heat conductivity of fiber assembly, λe (cal/cm·°C·s) is calculated by the following equation, when fibers are arranged at right angles :
    λe/λw=1/b(∞Σk-0) (-1) k (bn-βb-n) An
    And when fibers are arranged in equilaterally triangle shape, the above or following equation can be used :
    λe/λw=1/b(∞Σk-0)2An ((√a2+b2/2) n-β (√a2+b2/2) -n) sin nψ
    where,
    n=2k+1
    β=the parameter derived from the heat conductivities of fiber and medium
    λw=the heat conductivity of the medium (cal/cm·°C·s)
    a, b, ψ=the parameters depending on the arrangement of fibers in the fiber assembly
    An=the coefficients which satisfy the boundary conditions and can be obtained by applying the least squares method along the boundary lines
    The results calculated by these equations agreed well with experimental data and the results previously reported.
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  • K. Kawasaki
    1978 Volume 31 Issue 1 Pages P25-P30
    Published: January 25, 1978
    Released on J-STAGE: October 27, 2009
    JOURNAL FREE ACCESS
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  • Motivation in Clothing Selection
    M. Tanaka
    1978 Volume 31 Issue 1 Pages P31-P38
    Published: January 25, 1978
    Released on J-STAGE: October 27, 2009
    JOURNAL FREE ACCESS
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  • 1978 Volume 31 Issue 1 Pages P50-P72
    Published: January 25, 1978
    Released on J-STAGE: October 27, 2009
    JOURNAL FREE ACCESS
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