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Tetsu-to-Hagané Vol. 110 (2024), No. 2

ISIJ International
belloff

Grid List Abstracts
ONLINE ISSN: 1883-2954
PRINT ISSN: 0021-1575
Publisher: The Iron and Steel Institute of Japan

Backnumber

  1. Vol. 110 (2024)

    1. No.6
    2. No.5
    3. No.4
    4. No.3
    5. No.2
    6. No.1

  2. Vol. 109 (2023)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  3. Vol. 108 (2022)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  4. Vol. 107 (2021)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  5. Vol. 106 (2020)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  6. Vol. 105 (2019)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  7. Vol. 104 (2018)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  8. Vol. 103 (2017)

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    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  9. Vol. 102 (2016)

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    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    10. No.3
    11. No.2
    12. No.1

  10. Vol. 101 (2015)

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    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    10. No.3
    11. No.2
    12. No.1

  11. Vol. 100 (2014)

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    4. No.9
    5. No.8
    6. No.7
    7. No.6
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    11. No.2
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  12. Vol. 99 (2013)

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    5. No.8
    6. No.7
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    10. No.3
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    12. No.1

  13. Vol. 98 (2012)

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    5. No.8
    6. No.7
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  14. Vol. 97 (2011)

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    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    10. No.3
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    12. No.1

  15. Vol. 96 (2010)

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  16. Vol. 95 (2009)

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  17. Vol. 94 (2008)

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    5. No.8
    6. No.7
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  18. Vol. 93 (2007)

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    5. No.8
    6. No.7
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  19. Vol. 92 (2006)

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    5. No.8
    6. No.7
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  20. Vol. 91 (2005)

    1. No.12
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    3. No.10
    4. No.9
    5. No.8
    6. No.7
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  21. Vol. 90 (2004)

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    6. No.7
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  22. Vol. 89 (2003)

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    6. No.7
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  23. Vol. 88 (2002)

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    5. No.8
    6. No.7
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  24. Vol. 87 (2001)

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    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  25. Vol. 86 (2000)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    10. No.3
    11. No.2
    12. No.1

  26. Vol. 85 (1999)

    1. No.12
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    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  27. Vol. 84 (1998)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    10. No.3
    11. No.2
    12. No.1

  28. Vol. 83 (1997)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    10. No.3
    11. No.2
    12. No.1

  29. Vol. 82 (1996)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  30. Vol. 81 (1995)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  31. Vol. 80 (1994)

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    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    10. No.3
    11. No.2
    12. No.1

  32. Vol. 79 (1993)

    1. No.12
    2. No.11
    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    11. No.2
    12. No.1

  33. Vol. 78 (1992)

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    3. No.10
    4. No.9
    5. No.8
    6. No.7
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  34. Vol. 77 (1991)

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    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    11. No.2
    12. No.1

  35. Vol. 76 (1990)

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    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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  36. Vol. 75 (1989)

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    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
    8. No.5
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    10. No.3
    11. No.2
    12. No.1

  37. Vol. 74 (1988)

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    3. No.10
    4. No.9
    5. No.8
    6. No.7
    7. No.6
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  38. Vol. 73 (1987)

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    2. No.15
    3. No.14
    4. No.13
    5. No.12
    6. No.11
    7. No.10
    8. No.9
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    10. No.7
    11. No.6
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    14. No.3
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  39. Vol. 72 (1986)

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    2. No.15
    3. No.14
    4. No.13
    5. No.12
    6. No.11
    7. No.10
    8. No.9
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    10. No.7
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    14. No.3
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  40. Vol. 71 (1985)

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    2. No.15
    3. No.14
    4. No.13
    5. No.12
    6. No.11
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    10. No.7
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  41. Vol. 70 (1984)

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    3. No.14
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    5. No.12
    6. No.11
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  42. Vol. 69 (1983)

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    5. No.12
    6. No.11
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  43. Vol. 68 (1982)

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  44. Vol. 67 (1981)

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  45. Vol. 66 (1980)

    1. No.14
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    3. No.12
    4. No.11
    5. No.10
    6. No.9
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  46. Vol. 65 (1979)

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  47. Vol. 64 (1978)

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  48. Vol. 63 (1977)

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  49. Vol. 62 (1976)

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  50. Vol. 61 (1975)

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  51. Vol. 60 (1974)

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  52. Vol. 59 (1973)

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  53. Vol. 58 (1972)

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  54. Vol. 57 (1971)

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  55. Vol. 56 (1970)

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  56. Vol. 55 (1969)

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  57. Vol. 54 (1968)

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  58. Vol. 53 (1967)

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  59. Vol. 52 (1966)

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  60. Vol. 51 (1965)

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  61. Vol. 50 (1964)

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  62. Vol. 49 (1963)

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  63. Vol. 48 (1962)

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  64. Vol. 47 (1961)

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  65. Vol. 46 (1960)

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  66. Vol. 45 (1959)

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  67. Vol. 44 (1958)

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  68. Vol. 43 (1957)

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  69. Vol. 42 (1956)

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  70. Vol. 41 (1955)

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27 Apr. (Last 30 Days)

Tetsu-to-Hagané Vol. 110 (2024), No. 2

Analysis of Pulse-to-Pulse Signal Uncertainty in LIBS Spectral Intensity on the Basis of Error Propagation

Tetsuo Sakka, Yoshihiro Deguchi

pp. 35-40

DOI:

10.2355/tetsutohagane.TETSU-2023-083

Abstract

Atomic spectral lines obtained by laser-induced breakdown spectroscopy (LIBS) often suffer from serious pulse-to-pulse fluctuation, which limits the accuracy of the quantitative analysis. Solving this problem is an important issue for improving the analytical performance of LIBS. In the present review the model to simulate the emission spectral intensity of LIBS measurements is introduced, and the method to evaluate the propagation of the pulse-to-pulse variation of plasma parameters to the variation of emission spectral intensity by the error propagation analysis is explained. The recent three studies found in the literature that investigated the pulse-to-pulse fluctuation of the spectral line intensities on the basis of error propagation analysis are reviewed.

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Analysis of Pulse-to-Pulse Signal Uncertainty in LIBS Spectral Intensity on the Basis of Error Propagation

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Effect of the Jet from Top Lance on Slag Foaming Behavior in Basic Oxygen Furnace Process

Shinya Miura, Teppei Tamura, Ken-ichiro Naito

pp. 41-50

DOI:

10.2355/tetsutohagane.TETSU-2023-102

Abstract

As for steelmaking process such as basic oxygen furnace (BOF) and electric arc furnace (EAF), slag foaming consists of introducing gas bubbles into molten metal and slag by chemical reaction. In the case of the BOF process, excessive foaming is over the converter capacity, a phenomenon called “slopping”. Slopping reduces yield and equipment lifespan and increases production time. It is therefore important to control slag foaming properly. In previous studies by other investigators, the jet from top lance in BOF process effectively suppresses slag foaming. However, it is not obvious which mechanism of the jet from top lance is effective to suppress slag foaming, and its quantitative effect has not been reported. To clarify the relationship between slag foaming and the jet from top lance, the effects of the number of nozzle holes and lance height on the slag foaming were investigated by using a converter-shaped water-model device and test converter. The experimental results indicated that slag foaming height decreased as the number of nozzle holes increased. Also, slag foaming height changed instantly with the change in lance height, e.g., slag foaming height decreased as lance height increased, and vice versa. The foaming suppression mechanism of the jet from top lance is the entrainment of foaming slag into the jet. Consequently, slag foaming model that takes the effect of the jet from top lance into account is proposed. And it enables to predict the change in slag foaming height with time.

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Effect of the Jet from Top Lance on Slag Foaming Behavior in Basic Oxygen Furnace Process

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Cooling Condition to Prevent Thermal Stress Cracking during Slag Casting

Takeru Hoshino, Yasutaka Ta, Hiromu Yano, Hiroyuki Tobo

pp. 51-60

DOI:

10.2355/tetsutohagane.TETSU-2023-084

Abstract

Ferrous Slag Hydrated Matrix has been developed by mixing steel slag as aggregate. The direct casting process from molten slag was investigated instead of the complicated and expensive Matrix manufacturing process. However, cracks during casting can reduce strength. To prevent crack formation, the mechanism of thermal stress crack initiation and the appropriate conditions for casting molten slag in rock form were investigated by casting experiments, sound measurements, and thermal stress analysis. Compared with the slag cooled in the mold, the slag under the optimum cooling condition suppressed the cracks and did not cause cracks inside the slag. The crack sound was measured by sound measurements. To suppress the cracks, it was suggested that the temperature in the slag should be uniform quickly within 10 min after the slag injection. The required solidification shell thickness could be estimated based on the tensile stress generated on the slag surface. Through casting experiments and thermal stress analysis, cooling conditions to suppress thermal stress cracks in slag casting were revealed. In other words, it was found that when the molten slag is poured into the mold and then is demolded at the stage where the solidification shell thickness sufficiently exceeds the strength of the slag surface against the tensile stress applied to the solidification shell. The solidified slag is thermally insulated, and the temperature inside the slag is uniform. It cools while remaining uniform.

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Cooling Condition to Prevent Thermal Stress Cracking during Slag Casting

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Prediction Studies of Strip Centering with Flotation Dryer

Hirokazu Kobayashi, Yukio Takashima, Gentaro Takeda, Kenji Katoh, Tatsuro Wakimoto

pp. 61-71

DOI:

10.2355/tetsutohagane.TETSU-2023-082

Abstract

Flotation dryer systems are widely used to dry liquid layers on substrates such as films, paper and steel strips, and many reports discussing design optimization for better heat transfer characteristics and strip stability are available.

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Prediction Studies of Strip Centering with Flotation Dryer

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Effect of Nb on Grain Growth Behavior in the Heat Affected Zone of Linepipe Steels

Daichi Izumi, Nobuyuki Ishikawa, Pello Uranga, Nerea Isasti, Jose Maria Rodriguez-ibabe, Douglas Stalheim, David Jarreta, David Martin

pp. 72-82

DOI:

10.2355/tetsutohagane.TETSU-2023-096

Abstract

Recrystallization and grain growth during plate rolling are prevented by Nb addition both with the solute drag and the Nb carbide precipitation. Although a fine microstructure is achieved in the base material, welding heat completely changes the microstructure in the heat affected zone (HAZ). In this study, laboratory simulation of the coarse grain HAZ (CGHAZ) thermal cycle of double submerged arc welded linepipe was carried out using low carbon steels containing different Nb contents. Extraction residue analysis of the simulated CGHAZ samples revealed that almost all the Nb remained in solid solution. To clarify the interaction of Nb carbide dissolution and grain growth on overall simulated HAZ microstructure evolution, additional weld HAZ thermal simulations were performed. It was found that Nb carbides remain undissolved at HAZ peak temperatures up to 1200°C and showed significant pinning effect to prevent austenite grain growth. Significant grain growth was seen after continuous fast heating to 1350°C peak temperature, while the higher Nb added steel showed a slower overall austenite grain growth rate, suggesting that grain growth in the HAZ at higher temperature was suppressed by the combined effects of slower coarse Nb carbide dissolution providing some pinning, and the solute drag effect of higher amounts of Nb in solid solution. A pronounced retardation of longer-term isothermal grain growth was identified at 1350°C at higher levels of solute Nb, confirming the influence of Nb solute drag on high temperature resistance to austenite grain coarsening.

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Effect of Nb on Grain Growth Behavior in the Heat Affected Zone of Linepipe Steels

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Reverse Transformation Behavior in Multi-phased Medium Mn martensitic Steel Analyzed by In-situ Neutron Diffraction

Kyosuke Matsuda, Takuro Masumura, Toshihiro Tsuchiyama, Yusuke Onuki, Misa Takanashi, Takuya Maeda, Yuzo Kawamoto, Hiroyuki Shirahata, Ryuji Uemori

pp. 83-88

DOI:

10.2355/tetsutohagane.TETSU-2023-070

Abstract

The reverse transformation behavior during heating in Fe-10%Mn-0.1%C (mass%) martensitic alloy consisting of α’-martensite, ε-martensite and retained austenite was investigated using the in-situ neutron diffraction. When the temperature was elevated with a heating rate of 10 K/s, the ε→γ reverse transformation occurred first at the temperature range of 535–712 K, where Fe and Mn hardly diffused. In the temperature range where the ε→γ reverse transformation occurred, the full width at half maximum of the 200γ peak increased, indicating that the austenite reversed from ε-martensite contains high-density dislocations. In addition, the transformation temperature hardly depends on the heating rate and the crystal orientation of the reversed austenite was identical to that of the prior austenite (austenite memory), which suggests that the ε→γ reverse transformation would proceed through the displacive mechanism. After completion of the ε→γ transformation, the α’→γ reverse transformation occurred at the temperature range of 842–950 K. When the heating rate is low (<10 K/s), the reverse transformation start temperature significantly depends on the heating rate. It could be because the diffusional reverse transformation accompanying the repartitioning of Mn occurs. On the other hand, a higher heating rate (≥10 K/s) resulted in the disappearance of the heating rate dependence. This was probably due to the change in the transformation mechanism to the massive-type transformation, which is diffusional transformation without repartitioning of Mn.

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Reverse Transformation Behavior in Multi-phased Medium Mn martensitic Steel Analyzed by In-situ Neutron Diffraction

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