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Tetsu-to-Hagané
Vol. 92 (2006), No. 11

Tetsu-to-Hagané Vol. 92 (2006), No. 11

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

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Tetsu-to-Hagané Vol. 92 (2006), No. 11

Water Model Experiment on the Motion of a Non-spherical Particle in Molten Steel Based on Simultaneous Visualization of the Particle and Surrounding Flow

Goichi MATSUI, Manabu IGUCHI

pp. 643-648

Abstract

This study deals with the mechanism of small-body-falling namely the vortex-body interaction. The body is regarded as a model for nonmetallic inclusions moving or floating in molten steel. In the study visualization experiments for the motion of a small thin disk falling down in water have been conducted. The motion of the thin disk and its surrounding water velocity field were simultaneously measured using the MOFIA system. The velocity field around the disk was measured by particle image velocimetry (PIV). Fluorescent tracer particles with an average diameter of 10μm were used to separate the wavelengths from both that of YAG laser and those of lights for images taken by a CCD camera. The three dimensional motion of the disk was reconstructed using the images of two high-speed cameras. The experimental results collectively show that the motion of the disk was affected by its density and thickness. The motion changed from two-dimensional zigzag motion to spiral motion with an increase in the density of disk. In the case of a high density disk, a chaotic motion was observed.

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Water Model Experiment on the Motion of a Non-spherical Particle in Molten Steel Based on Simultaneous Visualization of the Particle and Surrounding Flow

Bibtex

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Reaction Mechanism between Solid CaO and FeO_x-CaO-SiO₂?P₂O₅ Slag at 1573K

Tasuku HAMANO, Shinya FUKAGAI, Fumitaka TSUKIHASHI

pp. 649-654

Abstract

Solid CaO and FeO_x-CaO-SiO₂-P₂O₅ slag were reacted for 2 to 2400 s at 1573K. The interface of CaO and slag was observed and analyzed by SEM/EDS. The CaO-FeO layer was formed beside solid CaO. The thickness of the CaO-FeO layer increased with time. Next to the CaO-FeO layer, 2CaO·SiO₂ phase was formed in the melt and high content of FeO was included in the liquid. The activities of FeO and CaO for each phase were evaluated and reaction mechanism between solid CaO and FeO_x-CaO-SiO₂-P₂O₅ slag was discussed. The activity of FeO for 2CaO·SiO₂ saturated melt is larger than that for the CaO-FeO layer, therefore, Fe²⁺ diffuses from slag phase to solid CaO. Then the CaO-FeO layer is formed beside solid CaO. The pass of the slag composition change accompanied by CaO dissolution are represented in the phase diagram for the FeO_x-CaO-(SiO₂+P₂O₅) pseudo ternary system.

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Reaction Mechanism between Solid CaO and FeO_x-CaO-SiO₂?P₂O₅ Slag at 1573K

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Flux Film in the Mold of High Speed Continuous Casing

Masahito HANAO, Masayuki KAWAMOTO

pp. 655-660

Abstract

The film, which is formed by mold flux in the continuous casting mold, plays very important roles in terms of lubrication or heat transfer.But, thickness or structure of it has not been adequately clarified.
In this study, it was tried to take the sample of actual flux film from the continuous casting mold just after the cast, keeping its position as it was during the cast. Thanks to this trial, thickness of the flux film at the meniscus in the mold could be clarified. According to the observation on the flux film section by microscope, the structure of the flux film was discussed, in terms of its crystallization.
Furthermore, based on the results of the observation mentioned above, the heat transfer phenomenon through the flux film in the mold was discussed.
As a result of the discussions, the following conclusions were obtained.
1) The mold flux film can be considered to be about 1 mm. Glassy layer, which has been considered to be molten flux on the top of molten steel during the cast and covered the film just after the cast, can be supposed to make up the film during the cast.
2) The liquid layer in the film is as thick as that is estimated on the basis of mold flux consumption during the cast.
3) In the case that the film at the meniscus in the mold is about 1 mm thick, total thermal resistance of radiation and conduction is equivalent to interfacial thermal resistance between the film and the mold.
4) The reported values of interfacial thermal resistance can be considered to be larger than that in the actual mold during the casting. The reason seems to be that they were measured in the condition without any pressure by the molten steel, like that in the mold. In the actual mold, the interfacial thermal resistance seems to be smaller.

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Flux Film in the Mold of High Speed Continuous Casing

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Deformation Analysis of Longitudinal Surface Micro-defects in Flat Rolling

Nobuki YUKAWA, Yoshinori YOSHIDA, Takashi ISHIKAWA

pp. 661-666

Abstract

The shape change of longitudinal surface micro-defects in flat rolling was investigated using a rigid-plastic finite element analysis. Rolling of plate with V-shaped scratches or rectangle defects that are parallel to the rolling direction, was simulated assuming a generalized plane strain condition. The calculated results were verified with experiments of model material, and good agreement between both results was obtained. The influence of rolling conditions, such as reduction, friction coefficient and the position of initial defect, on the shape of existing defect after rolling was evaluated. Using the developed FEM, the evolution of seam defects was also simulated, and good agreement with experimental results were obtained. The proposed prediction method can be utilized to make defect free products in flat rolling.

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Deformation Analysis of Longitudinal Surface Micro-defects in Flat Rolling

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Numerical Analysis of Cathodic Protection Distance for Steel-Zinc Couple under Thin Layer Electrolytes

Nobuhiro OKADA, Miki TAKEBAYASHI, Masamitsu MATSUMOTO, Masanari KIMOTO, Takeo KODOU

pp. 667-675

Abstract

Cathodic protection distance at the shear cut edge of zinc coated steel sheet is an important parameter for the lifetime of the steel material. However, cathodic protection distance is variable for electrolyte thickness, electric conductivity and so on. It is difficult to quantify the cathodic protection distance under various environmental conditions. So it is useful to estimate the cathodic protection distance by numerical analysis.
Most of numerical analysis models for galvanic corrosion use a polarization curve measured in a bulk electrolyte solution. However, under thin layer electrolytes, the cathodic current density strongly depends on the electrolyte thickness and the polarization curve shifts by salt concentration. So we developed the numerical analysis model that the polarization curve is calculated by the electrolyte thickness and NaCl concentration.
We investigated the cathodic protection distance in NaCl solution for several thicknesses and concentrations by numerical analysis. Moreover, we estimated the cathodic protection distance in the drying process of NaCl solution on the shear cut edge of zinc coated steel sheet.

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Numerical Analysis of Cathodic Protection Distance for Steel-Zinc Couple under Thin Layer Electrolytes

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Cross Cut Test for Coated Steel Plate

Yoshinobu NAKAMURA, Manabu ADACHI, Kazuya FUJITA, Yuta TACHIBANA, Takeo IIDA, Yoshiaki URAHAMA

pp. 676-682

Abstract

In order to develop the accuracy of cross cut test, some factors were investigated. Cellophane tape is widlely used in the cross cut test. It was found that the conditions of taping up, the peeling rate and angale must be accordance with JIS. While the temperature and humidity specifications during testing are described in JIS, a great care is required for storage, since the humindity has a strong influence on the performance of the pressure sensitive adhesives during storage as well as upon the results of a peel-off test. The fast rewinding rate from a reel of pressure sensitive adhesive tapes seem to make a rough surface. It must be noted these factors. The cellophase tape showed almost the same peel adhesion for various coated steel plates with different base and post coatings. Therefore, it was clarified that the cellophane tape is suitable for the cross cut test. The trench introduced by a cutter knife on the coated steel plate was observed by a laser microscope. In order to form the stable trench, it was found to be useful in accordance with JIS regulations except the blade angle at the trench introduction.

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Cross Cut Test for Coated Steel Plate

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Separation and Recovery of Phosphorus from Steelmaking Slags with the Aid of Strong Magnetic Field

Kazuyo YOKOYAMA, Hironari KUBO, Kazuhiro MORI, Hidehiko OKADA, Shuji TAKEUCHI, Tetsuya NAGASAKA

pp. 683-689

Abstract

In order to make sure the great potential of steelmaking slag as a new phosphorus resource, domestic phosphorus material flow in Japan including iron and steel industry has been investigated based on the statistical data on 2002. It has been demonstrated that phosphorus in the steelmaking slag is almost equivalent with that in the imported phosphate rock in the view points of the amount and the concentration. Phosphorus exists mainly in the form of calcium-phosphate or its solid solution with calcium-silicate rather than the Fe_tO rich liquid phase in the slag and exhibits remarkable segregation in the solidified slag. If the strong magnetic field is applied to the crushed slag, precipitated calcium-phosphate solution phase can be separated from Fe_tO matrix phase due to the large difference of each magnetic property. It has also been indicated by the Waste Input-Output model that the phosphorus recovery from steelmaking slag by the new process proposed in the present work has great environmental and economical benefits.

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Separation and Recovery of Phosphorus from Steelmaking Slags with the Aid of Strong Magnetic Field

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In-situ Observation of the Reduction of Iron Oxides by Solid State Carbon in TEM

Nobuhiro ISHIKAWA, Kazuo FURUYA, Takeshi AOYAGI, Nayuta MITSUOKA, Takashi INAMI

pp. 690-692

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In-situ Observation of the Reduction of Iron Oxides by Solid State Carbon in TEM

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Tetsu-to-Hagané Vol. 92 (2006), No. 11

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blast furnace

electoromagnetic

mg treatment inclusion

ステンレス鋼 ti-ni

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Tetsu-to-Hagané Vol. 92 (2006), No. 11

Water Model Experiment on the Motion of a Non-spherical Particle in Molten Steel Based on Simultaneous Visualization of the Particle and Surrounding Flow

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Reaction Mechanism between Solid CaO and FeOx-CaO-SiO2?P2O5 Slag at 1573K

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Flux Film in the Mold of High Speed Continuous Casing

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Deformation Analysis of Longitudinal Surface Micro-defects in Flat Rolling

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Numerical Analysis of Cathodic Protection Distance for Steel-Zinc Couple under Thin Layer Electrolytes

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Cross Cut Test for Coated Steel Plate

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Separation and Recovery of Phosphorus from Steelmaking Slags with the Aid of Strong Magnetic Field

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In-situ Observation of the Reduction of Iron Oxides by Solid State Carbon in TEM

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Article Access Ranking

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Perspectives on the Promising Pathways to Zero Carbon Emissions in the Steel Industry toward 2050

New Electromagnetic Flow Control System for Optimization of Molten Steel Flow in Continuous Casting Mold

Preface to the Special Issue on “Challenges to Comprehension for Phenomena of Degradation, Softening, and Melting of Raw Materials in Hydrogen-enriched Ironmaking Process”

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Effect of Al in the coating layer of Zn-coated steel sheet on Zn oxidation during hot-stamping heating

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Reaction Mechanism between Solid CaO and FeO_x-CaO-SiO₂?P₂O₅ Slag at 1573K

Ammonia as a Green Energy Carrier to Lower Blast Furnace CO₂ Emissions