Sen'i Gakkaishi
Online ISSN : 1884-2259
Print ISSN : 0037-9875
Volume 12, Issue 1
Displaying 1-11 of 11 articles from this issue
  • Tokiji Narita
    1956Volume 12Issue 1 Pages 2-5
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
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  • (1) THE METHOD OF MEASURING THE LATERAL ORDER DISTRIBUTION IN REGENERATED CELLUL (2) THE LATERAL ORDER DISTRIBUTION OF SEVERAL HIGH TENACITY RAYONS
    Hirokuni Maeda
    1956Volume 12Issue 1 Pages 6-13
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
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  • Nobuhiko Migita, Takashi Kanda, Shuichi Sato, Yukio Kojima
    1956Volume 12Issue 1 Pages 14-18
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
    The effect of hemicellulose contents in pulp on beating rate and strength of paper made from it was studied.
    In this study two methods were used, one the adding method (adding isolated hemicellulose to the standard pulp) and the other the extracting method (removing hemicellulose stepwisely).
    In the former when the hemicellulose is isolated with drastic agents, chemical nature of hemicellulose is liable to change, so that it is impossible to say that the isolated hemicellulose will act in the same manner as it does in the original state. Therefore extracting method was employed in the present research.
    For the preparation of chlorite holocellulose, thin pieces of beech and aspen wood were treated with hot acidified sodium chlorite. These chlorite holocelluloses were treated with KOH solution under nitrogen gas, in order to minimize the oxidation of cellulose. For hemicellulose extraction, KOH solutions of various concentration (from 0.3 to 20%) were used in order to get a series of pulp in which the hemicellulose content was stepwisely arranged.
    The beating rate and the sheet strength of this series of pulp were examined. From the result of this study, it was concluded that there appeared to be the optimum hemicellulose content in pulp as for as the paper strength was concerned. Other observations were also made with regard to the result observed.
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  • (IV) ON THE VELOCITY OF THE INDIVIDUAL FIBER (V) ON THE SITUATION AND THE RANGE OF THE DISTRIBUTION FOR THE VELOCITY-CHANGE-POINTS
    Shuichi Ichino, Shinya Kurosaki
    1956Volume 12Issue 1 Pages 19-23
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
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  • (IV). ON THE CONTRACTIVE FORCE OF TWISTED FIBER FILAMENT
    Keiroku Fuchino, Yasuo Sunaga, Hiroshi Nakamichi
    1956Volume 12Issue 1 Pages 24-27
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
    The difference between the ideal contractive force of a multifilament with circular section and the observed value of corresponding monofilament by twisting at a fixed length may be explained by the fineness of the fiber included in the multifilament.
    If the denier of the monofilament is known, the number of corresponding multifilament of various denier of fiber can be calculated by the following formula._??_
    where R; Diameter of multifilament equal to the cross section of Amilan or Saran under consideration. r; Diameter of fiber included in these multifilament. n; Number of fiber.
    The curve between contractive force at break of these multifilament by twist under a fixed length and their denier of fiber are shown in Figs 4 & 5.
    From these curves and observed values, we can estimate the fineness of fiber (Fibrill) for Amilan (890 D); Saran (1146 D) which correspond respectively to 3 d, 18 d.
    Especially for Saran, the fineness of fiber 18 d (Fibrill) is ascertained by microscopic observation.
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  • (I) THEORETICAL AND EXPERIMENTAL STUDIES ON THE WINDING YARN CURVES AROUND THE WEFT PIRNS
    Hosaku Uchida, Eiichi Kuze, Keijiro Hyodo, Tetsuya Sakai
    1956Volume 12Issue 1 Pages 28-32
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
    Findings of theoretical and experimental researches on the winding yarn cnrves around the weft pirns are reported.
    The displacement Z of the contact point between yarn and pirn or yarn layer surface along the pirn's central axis is calculated by the following equation;
    where, form of pirn or yarn layer is cylindrical, spindle, revolving speed is constant and traversing motion of yarn guide is expressed by A (1-cosKw).
    w: revolving angle of the spindle
    r: radius of the cylindrical pirn or yarn layer
    d: distance between the pirn or yarn layer surface and traversing yarn guide
    A: amplitude of a traverse
    K: speed ratio between the traverse motion and spindle revolution
    If the pirn or yarn layer is conical form;
    where r: mean radius of the pirn or yarn layer
    In the equations (1) and (2) above, the first term expreses the traverse motion and the second term expreses the deflection between the yarn motion around the pirn and the yarn guide motion.
    It is noted that the focuses of the weft yarn curves around the pirn obtainied by the experimental method almost coincide with the calculation by the equations (1) & (2), and the larger d and K are the large becomes the deflection between the yarn motion around the pirn and the yarn guide motion.
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  • (III) SOME SUGGESTIONS TO IMPROVE THE APPARATUS AND TO SIMPLIFY THE TEST PROCEDURE
    Hosaku Uchida, Toru Takizawa, Mitsuru Kobayashi
    1956Volume 12Issue 1 Pages 33-40
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
    The authors continued the experimental study to improve the ring part and to simplify the test procedure. The results are briefly reported as follows:
    1. Instead of hard-chrome plated steel ring, rubber rings of the same size were put to test in anticipation of obtaining more reasonable and practical results, because of its softness and elastic properties resembling those of human fingers. But the rubber ring gave neither such desired results nor any feasable outcome.
    2. For the purpose of obtaining a simpler expression of withdrawal resistance without troublesome calculations, the authors used an idea of “mean withdrawal resistance per unit sectional area.”
    mean with drawal resistance per unit sectional area Fm/Afm
    where Fm: mean withdrawal resistance over a range of fullness from 0 to x, x_??_1.0 A: sectional area of ring hole.
    In a range of fullness up to 1.0, the value of fm practically coninside with the result calculated from the experimental formula, αρβ, in the previous report.
    3. A trial to obtain values of fm that would coninsided of various diameter of ring holes by using a series of ring holes of similar dimensions, ended in a failure. In this case also, the same test piece gives different values of fm if tested by rings of different diameter.
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  • (2) THE SLIPPAGE OF THE WORSTED AND WOOLEN FABRICS (3) THE KINETIC FRICTION OF FABRICS
    Yoshito Miura
    1956Volume 12Issue 1 Pages 41-47
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
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  • (1) THE DISSOCIATION ENERGY OF DIRECT DYE-FIBER-COMPLEX
    Yukio Konishi, Kosaku Shibata
    1956Volume 12Issue 1 Pages 48-53
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
    Dye accessibility of fiber depends on the magnitudes of the following factors:
    1. The surface area through which the dye passes into the fiber.
    2. The speed by which the dye migrates in the fiber.
    3. The inner volume υ (cc. per lg dry fiber) in which the dye exists.
    4. The dissociation energy E of the dye-fiber-complex.
    As (1) and (2) can be calculable when E is known, the author starts the studies from obtainingE.
    When in the hot and very dilute direct dye solution the sizes of the dye particles are very small and homgeneous, there holds the next relation. (dissociation energy of a dye particle from the dyed fiber) (cal/ particle) Here k: Boltzmann's constant, T: absolute temperature, m0: number of dye particles in the initial dye bath, m: number of dye particles in the equilibrium reaching dye bath, υ: volume of the dye bath.
    The dyeing experiments are as follows.
    Materials to be dyed; viscose rayon, cuprammonium rayon, Vinylon (appolyvinylformal fiber), and polyvinylalcohol fiber. Temperature: 80°C Period: 3 hrs. Liquor ratio: 1/250. Dyes: Benzopurpurine 4BKX Chrysophenine NS Naphthamine Blue 12B (all purified). Dye concentration: 0.001%(Wt) (Benzopurpurine 0.003%) NaCl concentration: 0.001%(Wt) (Benzopurpurine 0.0003%) The results are:
    Under the same dyeing condition E of Vinylon is found to be greater than that of cellulose fiber. but smaller than that of polyvinylalcohol fiber.
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  • Naosuke Akagawa
    1956Volume 12Issue 1 Pages 54-58
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
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  • Hideichi Matsuda
    1956Volume 12Issue 1 Pages 59-65
    Published: January 10, 1956
    Released on J-STAGE: November 28, 2008
    JOURNAL FREE ACCESS
    Download PDF (566K)
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