Tetsu-to-Hagane
Online ISSN : 1883-2954
Print ISSN : 0021-1575
ISSN-L : 0021-1575
Volume 80, Issue 11
Displaying 1-12 of 12 articles from this issue
  • Yoshikiyo OGINO
    1994 Volume 80 Issue 11 Pages 807-812
    Published: November 01, 1994
    Released on J-STAGE: January 18, 2010
    JOURNAL FREE ACCESS
    Download PDF (1332K)
  • Kenji ANDO, Kazuhiko IWAI, Shigeo ASAI
    1994 Volume 80 Issue 11 Pages 813-818
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    A new method for pouring a molten charge out of a levitation type cold crucible has been proposed. In the new method, the charge is taken out through the bottom-hole of the crucible by changing the magnetic field which results in the break-down of the mechanical balance among magnetic pressure, hydrostatic pressure and the pressure due to surface tension. Pouring the charge out of the crucible was demonstrated by changing the distance between the coil and the crucible. A new technique which can fix the shape of the molten charge in the crucible has been proposed. By using this technique, the elongation of the charge shape predicted by the numerical analysis was confirmed and whether the charge contacted with the crucible was examined. In the experiment, the small temperature difference between the molten charges before and after pouring was observed and the large super heat in the poured metal was available.
    Download PDF (8146K)
  • Minoru SASABE, Hidekiyo ITAKURA
    1994 Volume 80 Issue 11 Pages 819-824
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    Annual production rates of crude steel of various countries in future are estimated by the following procedure : First, real production rates are corrected by a regular procedure. Then equations of relationship between the corrected production rate and the year are expressed by regression of a logistic equation. Estimated production in various countries can be obtained by subtracting the difference of the corrected and the real productions from the regressed amount.
    For examples of results, the maximum production rate of Japan in future can be estimated as 120Mt/y. It is also suggested that annual production rate under depression in near future can be estimated.
    Download PDF (978K)
  • Mitsutaka HINO, Ken-ichi HIGUCHI, Tetsuya NAGASAKA, Shiro BAN-YA
    1994 Volume 80 Issue 11 Pages 825-830
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    The activity of iron chromite in solid FeO·Cr2O3-MgO·Cr2O3-MgO·Al2O3 spinels, saturated with (Cr, Al)2O3, was determined at 1573 K, by the equilibrium of iron dissolved into liquid silver in the spinel crucible with CO-CO2gas mixture, to clarify the thermodynamic properties of chromium ores used in ferrochromium industry.
    The phase relation between (Cr, Al)2O3and FeO·Cr2O3-MgO·Cr2O3-MgO·Al2O3spinel phase was studied, and the solubility of (Cr, Al)2O3 in FeO·Cr2O3MgO·Al2O3, MgO·Cr2O3-MgO·Al2O3 and FeO·Cr2O3-MgO·Cr2O3-MgO·Al2O3 spinel phases was found to be small.
    The activity of FeO·Cr2O3 in FeO·Cr2O3-MgO·Cr2O3-MgO·Al2O3spinel solid solution coexisted with (Cr, Al)2O3shows negative deviation from ideality. It was observed that the spinel solid solution took regular solution behavior, and α-function of each pseudo-binary in FeO·Cr2O3-MgO·Cr2O3-MgO·Al2O3system was determined as follows;
    α FeO·Cr2O3-MgO·Al2O3=-92, 000(J),
    αMgO.Cr2O3-MgO·Al2O3=-30, 000 (J)
    Download PDF (1177K)
  • Kazumi YASUDA, Hiroyuki KAJIOKA
    1994 Volume 80 Issue 11 Pages 831-836
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    Cooling rate is an important index to estimate solidification structure or property of cast products.
    In order to evaluate the upper limit of the cooling rate in near net shape casting processes of various kinds, heat conduction in the semi-infinite region with and without solidification was calculated analytically. On the basis of Neumann's solution for the semi-infinite region (y>0) initially at constant temperature U with the surface (y=0) maintained at zero for the subsequent time (t>0), cooling rate was calculated for the cases in which location, time or temperature was fixed respectively.
    The results are as follows.
    (1) In case of cooling without solidification, the maximum cooling rate at any fixed location takes place at the constant temperature 0.92U independent of the thermal characteristics. While in case time is fixed, the maximum cooling rate occurs at another constant temperature of 0.68U.
    (2) In case of cooling with solidification, cooling rate is determined by location, time and the dimensionless parameter Ya, which is the ratio between sensible and latent heat, And for any kind of metal the maximum cooling rate at any fixed location or time appears just behind the solidification front. Approximate equations for the maximum cooling rate are proposed.
    Download PDF (1040K)
  • Kazumi YASUDA, Hiroyuki KAJIOKA
    1994 Volume 80 Issue 11 Pages 837-842
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    It has been difficult to get an analytical solution for temperature distribution in a solidifying and cooling process in a mold of continuous casting machine, because of multi-layered heat resistance between solidification front and water cooling surface of a mold ; solidified shell/ melt or solidified powder/ air gap/ mold coating/ mold metal and cooling water. Numerical methods, which are inconvenient to get a perspective of the total system, have been the only measure to analyse processes.
    The object of this research is to present a new general method to analyse a mold cooling system.
    The authors proposed a new concept "quasi-steady state", and defined a new standard function "cast function" as a solution of a linear heat flow model. They established a new precise general method to analyse a mold cooling system. As a result it has become possible to express explicitly temperature at arbitary location and time in the casting and cooling system.
    They also made a comparison among this method and other model methods.
    Download PDF (1112K)
  • Kuniaki MARUOKA, Tsuyoshi KAWANO, Yasuhiko YAMASHITA
    1994 Volume 80 Issue 11 Pages 843-848
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    The possibility was fundamentally investigated, that the demand to light weight DWI can could be satisfied by bake-hardenable and thin gauge tinplate which had excellent DWI formability at the stage of DWI forming before baking and had high pressure resistance after baking due to such bake-hardenability as automotive steel sheets.
    At first, change of mechanical property of continuous annealed tinplate with controlled amount of solute carbon due to forming was experimentally investigated by simulating DWI forming by cold rolling. Such tinplate showed increase of yield strength due to bake-hardening following cold rolling corresponding to bottom forming, and that was expected to improve dome pressure resistance. At the same time, since tensile strength of bake-hardenable tinplate cold rolled up to 70% was not higher than that of conventional tinplate, DWI formability of bake-hardenable tinplate was expected to be equivalent to that of conventional one.
    Then model cans were experimentally manufactured from 2 types of tinplate, and the improvement of dome pressure resistance in bake-hardenable tinplate was proved.
    Finally it was discussed that dome was fully reinforced by structural design and that the burst of dome was considered a kind of plastic collapse.
    Download PDF (1028K)
  • Hikaru OKADA, Tomoki FUKAGAWA, Haruhiko ISHIHARA, Atsuki OKAMOTO, Masa ...
    1994 Volume 80 Issue 11 Pages 849-854
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    Red scale defects usually observed in high Si hot rolled strip were reproduced in a laboratory 3 stand tandem mill. The effects of hot rolling and descaling condition on the strip surface color and scale structure were examined.
    Irrespective of Si content in steel, the hot rolled strip surface became red when the scale thickness before rolling was above 20μm and the rolling temperature was below 900°C. It was found that surface part of the scale (mainly FeO) was broken to powder by the hot rolling at the temperature below 900°C. The red scale of Fe2O3 was formed by the oxidation of powdered scale during cooling. Thick scale formed during slab soaking was completely removed by hydraulic descaling before rolling in low Si steel, whereas that was not removed in high Si steel. This remained scale caused the red scale defects after rolling and cooling. The application of obtained results to the hot strip mill production of red scaleless strip was discussed.
    Download PDF (7086K)
  • Nobukazu SUZUKI, Nobuyuki ISHII, Yutaka TUCHIDA
    1994 Volume 80 Issue 11 Pages 855-859
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    Diffusible hydrogen behavior in pre-strained high strength steel was investigated by use of a newly developed hydrogen content determining method for better understanding of delayed fracture.
    Pre-straining up to 4.2% formed a new hydrogen trapping site in the steel. When hydrogenerated in a 0.1N HCl solution, hydrogen content in the steel increased with the amount of pre-straining. The trapping site resulted from prestraining was removed by aging at 200°C.
    During the hydrogenation of the 4.2% pre-strained specimen, hydrogen content in the steel increase in accordance with Fick's law.
    The decrease of hydrogen content in the specimen pre-strained, hydrogenated, then held at room temperature cannot be explained by a single diffusion rate. This phenomenon can be better explained by assuming that hydrogen in the lattice and trapping sites diffuse independently without showing local equilibrium.
    Download PDF (867K)
  • Takashi KATSURAI, Tatsumi TOZAWA, Hajime KATO, Yoshimasa TAKAYAMA
    1994 Volume 80 Issue 11 Pages 860-865
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    A metallic gasket for the cylinder head of the automobile engine is made of an austenitic stainless steel sheet. It commonly has a press-formed bead which seals the high pressure gas in the combustion chamber. Because the fatigue characteristics of the sheet with the bead do not correspond to those of the plain sheet without bead, it is not easy to judge the suitability of the materials for the metallic gasket. We investigated the fatigue behavior for the sheet with the bead, especially the number of crack origins and the fatigue crack propagation rate. As a result, the fatigue strength at the number of 106 cycles was not dependent on the mean stress but the stress amplitude. In addition, the discrepancy between the fatigue characteristics of the sheets with and without the bead resulted from fine wrinkle-like bands of plastic deformation which occurred at a part of bead profile foot during the bead-forming.
    Download PDF (5502K)
  • Masahiko IKEDA, Shin-ya KOMATSU, Takashi SUGIMOTO, Kiyoshi KAMEI, Koic ...
    1994 Volume 80 Issue 11 Pages 866-870
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    Previous results on β quenched Ti-215%(mass%) Fe alloys suggested that the volume fraction of athermal ω phase (ωath) was maximum in the Ti-5%Fe alloy. In present work, influence of Al addition to the Ti-5%Fe alloy on the formation of ωath has been investigated by resistivity and hardness measurement, X-ray and electron diffractometry in the β quenched state.
    In alloys containing up to 8%Al, optical microscopy reveals single phase structure, and only β phase is detected by X-ray diffraction.
    Resistivity monotonously increases with Al content. Resistivity ratio between liquid nitrogen and room temperature, ρLNRT, shows a maximum at 6%Al, at which hardness shows a minimum.
    Room temperature electron diffraction pattern due to athermal ω phase is changed by the Al addition from clear spots to diffuse scattering.
    Similarly as the case of Ti-20V-Al, it is considered that the added Al dissolves substitutionally into β Ti-5%Fe lattice, lowers starting and finishing temperatures of athermal ω phase formation, ωS and ωf, and then decreases volume fraction of athermal ω phase at room temperature.
    Download PDF (6325K)
  • Yotaro OHNO
    1994 Volume 80 Issue 11 Pages N558-N563
    Published: November 01, 1994
    Released on J-STAGE: June 19, 2009
    JOURNAL FREE ACCESS
    Download PDF (1382K)
feedback
Top