logo
Language
Bookmarks
Log Out

Journals

Search Sites

Account

© 2022 Steel Science Portal

How to use

Advanced Search

Search Sites

site
site
site
site

ISIJ International Vol. 44 (2004), No. 3

ISIJ International
belloff

Grid List Abstracts
ONLINE ISSN: 1347-5460
PRINT ISSN: 0915-1559
Publisher: The Iron and Steel Institute of Japan

Backnumber

  1. Vol. 64 (2024)

    1. No.13
    2. No.12
    3. No.11
    4. No.10
    5. No.9
    6. No.8
    7. No.7
    8. No.6
    9. No.5
    10. No.4
    11. No.3
    12. No.2
    13. No.1

  2. Vol. 63 (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. 62 (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. 61 (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. 60 (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. 59 (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. 58 (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. 57 (2017)

    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

  9. Vol. 56 (2016)

    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

  10. Vol. 55 (2015)

    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

  11. Vol. 54 (2014)

    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

  12. Vol. 53 (2013)

    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

  13. Vol. 52 (2012)

    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

  14. Vol. 51 (2011)

    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

  15. Vol. 50 (2010)

    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

  16. Vol. 49 (2009)

    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

  17. Vol. 48 (2008)

    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

  18. Vol. 47 (2007)

    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

  19. Vol. 46 (2006)

    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

  20. Vol. 45 (2005)

    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

  21. Vol. 44 (2004)

    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

  22. Vol. 43 (2003)

    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

  23. Vol. 42 (2002)

    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
    13. No.Suppl

  24. Vol. 41 (2001)

    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
    13. No.Suppl

  25. Vol. 40 (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
    9. No.4
    10. No.3
    11. No.2
    12. No.1
    13. No.Suppl

  26. Vol. 39 (1999)

    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

  27. Vol. 38 (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
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  28. Vol. 37 (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
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  29. Vol. 36 (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
    13. No.Suppl

  30. Vol. 35 (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. 34 (1994)

    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

  32. Vol. 33 (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
    9. No.4
    10. No.3
    11. No.2
    12. No.1

  33. Vol. 32 (1992)

    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

  34. Vol. 31 (1991)

    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

  35. Vol. 30 (1990)

    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

  36. Vol. 29 (1989)

    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

Keyword Ranking

21 Nov. (Last 30 Days)

ISIJ International Vol. 44 (2004), No. 3

Macroscopic Models for Gas Stirred Ladles

D. Mazumdar, J. W. Evans

pp. 447-461

DOI:

10.2355/isijinternational.44.447

Abstract

Considerable efforts have been made during the past two decades to develop reliable and effective macroscopic process models for inert gas stirred ladles. The primary objective of these has been to develop simplified equations/expressions embodying a set of key operating variables such as ladle dimensions, gas flow rate, nozzle/tuyère dimension and so on for hydrodynamics, scaling criterion, structure and profiles of the gas-liquid two phase plume, mixing, heat and mass transfer between solids and bulk liquid etc. An exhaustive literature search on the subject indicates that both fundamental as well as empirical approaches were adopted by investigators to develop these simplified process models. It was further noted that a vast majority of these studies applied aqueous model of gas stirred ladle systems as a means to arrive at or validate such models. Parallel to this, limited available evidence within the literature also suggests that macroscopic models, despite being simplistic have a sound basis and therefore can form a reasonably reliable predictive framework, particularly in the absence of any elaborate computer solutions, for first hand analysis of rate processes in gas stirred ladles.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Macroscopic Models for Gas Stirred Ladles

twitter
facebook
mendeley

Bibtex

Ris

Reduction Behaviour of Iron Ore Fluxed Pellets under Load at 1 023-1 273 K

A. A. El-Geassy, M. I. Nasr, M.H. Khedr, K. S. Abdel-Halim

pp. 462-469

DOI:

10.2355/isijinternational.44.462

Abstract

Commercially, high grade acidic and basic fluxed iron ore pellets were isothermally reduced at 1 023-1 273 K under different load values ranging from 0.0 up to 0.0559 MPa. The reduction was carried out with synthetic gas mixture containing 55 vol% H2, 36 vol% CO, 5 vol% H2O, 3 vol% CO2 and 1 vol% N2. The oxygen weight loss resulted from the reduction of Fe2O3 to lower oxides or to metallic iron was continuously recorded as function of time. X-ray phase analysis, optical microscope, high-pressure mercury porosimeter were used to characterise fluxed and reduced pellets. The different parameters affecting the reduction of these pellets were studied and correlated. It was found that the basicity of pellets (CaO+MgO)/(SiO2+Al2O3) is 0.37 and 1.62. At early and intermediate stages, the reduction increased gradually with temperature showing a significant increase in the rate at >1 173 K. At later reduction stages, the load had a measurable effect on the reduction due to the sintering of freshly reduced metallic iron that increased with temperature and reduction extent. The internal structure was correlated with the reduction kinetics to predict the corresponding mechanism. The inter-relating effect of temperature and load on the reduction kinetics of fluxed pellets was also given.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Reduction Behaviour of Iron Ore Fluxed Pellets under Load at 1 023-1 273 K

twitter
facebook
mendeley

Bibtex

Ris

Influence of Lime/Limestone Addition on the SO2 and NO Formation during the Combustion of Coke Pellet

Man-Seung Lee, Sang-Chul Shim

pp. 470-475

DOI:

10.2355/isijinternational.44.470

Abstract

Isothermal combustion experiments of coke pellet mixed with lime/limestone had been performed to investigate the effect of lime/limestone addition on the reduction of NO and SO2 emission. The coke pellets were combusted between 700°C and 1300°C under pure oxygen atmosphere. Combustion kinetics and conversion data of SO2 and NO were obtained from the thermogravimetry of coke pellet and gas analysis data. Adsorption of NO by lime mixed with coke was not occurred in the experimental ranges. It was possible to reduce most of SO2 emission below 900°C by adding lime/limestone to coke. However, the reduction efficiency of SO2 by the addition of lime/limestone decreased with increasing temperature due to the decomposition reaction of CaSO4. The variation of the conversion to NO and SO2 with the combustion conditions during the combustion of coke pellet was compared with the results of thermodynamic calculation.

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Influence of Lime/Limestone Addition on the SO2 and NO Formation during the Combustion of Coke Pellet

twitter
facebook
mendeley

Bibtex

Ris

Phase Equilibria of Two-liquid CaO-MgO-FetO-P2O5 Slag Saturated with (Mg, Fe)O

Teppei Tamura, Tetsuya Nagasaka, Mitsutaka Hino

pp. 476-481

DOI:

10.2355/isijinternational.44.476

Abstract

Phase equilibria of two-liquid CaO-MgO-FetO-P2O5 slag saturated with (Mg, Fe)O solid solution and the distribution ratio of phosphorus between the slag and liquid iron were measured at steelmaking temperatures by chemical equilibration. It is known that this slag system has wide liquid miscibility gap at steelmaking temperature and this two-liquid phase slag has many advantages, such as high activities of both FetO and CaO and high amount of phosphoric oxide. It was made clear that the phosphorus distribution ratio between the slag system and molten iron was higher than that of the CaOsat.-FetO-P2O5 system and the two-liquid slag phase was very useful for dephosphorization of molten steel and reduction of slag volume.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Phase Equilibria of Two-liquid CaO-MgO-FetO-P2O5 Slag Saturated with (Mg, Fe)O

twitter
facebook
mendeley

Bibtex

Ris

Swelling Behaviour of Cement-bonded Briquettes-proposed Model

Maneesh Singh, Bo Björkman

pp. 482-491

DOI:

10.2355/isijinternational.44.482

Abstract

The cement-bonded agglomeration process is an alternative to the traditional balling-sintering process for recycling iron-rich by-products generated in iron and steel plants back to the blast furnaces. It has been observed that, under certain conditions, the briquettes containing pellet-fines show a tendency to swell catastrophically when reduced. This swelling is dependent upon a number of factors like: reducing temperature, composition of briquettes, particle size of raw material, amount of cement and composition of reducing gas. The SEM and optical micrographs do not show the formation of iron whiskers as the cause of swelling; instead, the swelling is due to the movement of reduced iron particles away from each other. It has been proposed that the swelling takes place in three steps: (a) fragmentation of weak pellet-fines particles during reduction to wustite; (b) formation of liquid slag due to reaction between CaO, MgO, FeO, SiO2 and Al2O3; (c) generation of high gas pressure due to formation and subsequent oxidation of metastable iron carbide.

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Swelling Behaviour of Cement-bonded Briquettes-proposed Model

twitter
facebook
mendeley

Bibtex

Ris

Modeling of Combustion and Heat Transfer in an Iron Ore Sintering Bed with Considerations of Multiple Solid Phases

Won Yang, Changkook Ryu, Sangmin Choi, Eungsoo Choi, Deokwon Lee, Wanwook Huh

pp. 492-499

DOI:

10.2355/isijinternational.44.492

Abstract

The iron ore sintering was characterized as a relatively uniform process of solid material, coke combustion, various modes of heat transfer, and the complicated physical changes of solid particles. The sintering bed was modeled as an unsteady one-dimensional process of the solid materials with multiple solid phases, which confers a phase on each kind of solid material. Each solid phase had a specific particle size and compositions. Drying, condensation, coke combustion, limestone decomposition, generation of the macroscopic internal pore and shrinking of the bed were considered. Complicated modes of heat transfer including conduction, convection and radiation were considered. Numerical simulations of the condition in the iron ore sintering bed were carried out for various parameters: coke contents and air suction rates, along with some other parameters of the model. Calculation results were compared with the results of the sintering pot test. The temperature profiles and gas compositions showed a good agreement with the experimental data.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Modeling of Combustion and Heat Transfer in an Iron Ore Sintering Bed with Considerations of Multiple Solid Phases

twitter
facebook
mendeley

Bibtex

Ris

Numerical Investigation on Effects of Deadman Structure and Powder Properties on Gas and Powder Flows in Lower Part of Blast Furnace

Hiroshi Nogami, Peter Richard Austin, Jun-ichiro Yagi, Kazuyoshi Yamaguchi

pp. 500-509

DOI:

10.2355/isijinternational.44.500

Abstract

Deposition of excessive amount of fine powder in the lower part of blast furnace deteriorates permeability of packed bed for reacting gas and liquid products, and causes operation instability. Powder behavior in the lower part of blast furnace has been attracting technical and scientific interests with increase in injection rate of pulverized coal into blast furnace. This study performed numerical experiments on effects of deadman structure and properties of generated powder on gas and powder flow behavior in the lower part of blast furnace by using two-dimensional axisymmetric mathematical model for flow and heat transfer in blast furnace based on multi-fluid theory. Among the packed bed properties, voidage has greater effect than coke diameter on penetration of high temperature gas and powder into the deadman zone and pressure drop in the furnace. The deadman having extremely low voidage is possibly to cause formation of low temperature zone in the deadman. Thus it is preferable to repress powder accumulation within deadman packed bed to keep its permeability. Increase in powder diameter raises the maximum value of volume fraction of powder within the deadman, and heavier particles tend to leave from the gas stream. Such particles are considered easy to accumulate in the deadman. Therefore decrease in generation of larger and heavier particles and increase in their consumption are effective to realize permeable deadman.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Numerical Investigation on Effects of Deadman Structure and Powder Properties on Gas and Powder Flows in Lower Part of Blast Furnace

twitter
facebook
mendeley

Bibtex

Ris

Numerical Analysis on Charging Carbon Composite Agglomerates into Blast Furnace

Mansheng Chu, Hiroshi Nogami, Jun-ichiro Yagi

pp. 510-517

DOI:

10.2355/isijinternational.44.510

Abstract

The carbon composite agglomerates have been numerically examined. The previously presented multi-fluid blast furnace model is modified to simulate blast furnace operation with carbon composite agglomerates charging. The model considers the behavior of carbon composite agglomerates, namely, conservation equations of chemical species contained in this material including chemical reactions and phase transformations are newly added. A series of simulating calculations are performed to examine the effect of charging carbon composite agglomerates. The result reveals that with increase in carbon composite agglomerates charging ratio in-furnace temperature level tends to decrease, the location of cohesive zone shifts downward, and the reductions of carbon composite agglomerates and sinter are delayed. On the other hand, the productivity tends to increase while coke rate and total reducing agent rate show decrease. The energy consumption for unit production of hot metal is lowered. The performance of blast furnace is improved in the tested range mainly due to the decrease in heat requirements for solution loss, sinter reduction and silicon transfer reactions, heat outflow by top gas and wall heat loss.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Numerical Analysis on Charging Carbon Composite Agglomerates into Blast Furnace

twitter
facebook
mendeley

Bibtex

Ris

Mathematical Model of Gas Flow Distribution in a Scale Model of a Blast Furnace Shaft

Juan Jiménez, Javier Mochón, Jesús Sainz de Ayala

pp. 518-526

DOI:

10.2355/isijinternational.44.518

Abstract

The mutual influence between gas flow and burden distribution in the upper part of a blast furnace has been studied employing a simplified mathematical model to estimate burden distribution and a gas flow model based on Ergun's equation.
Experiments carried out on a 1/10 scale cold model of Aceralia's blast furnace B were compared with results obtained from these mathematical models. Results corroborate that changes in burden distribution during the charging process have a strong influence on gas distribution, which also affects the burden layer profiles. These interrelations should be taken into account when the blast furnace charging patterns are designed

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Mathematical Model of Gas Flow Distribution in a Scale Model of a Blast Furnace Shaft

twitter
facebook
mendeley

Bibtex

Ris

Computer Applications of Thermodynamic Databases to Inclusion Engineering

In-Ho Jung, Sergei A. Decterov, Arthur D. Pelton

pp. 527-536

DOI:

10.2355/isijinternational.44.527

Abstract

Computerized thermodynamic databases for solid and liquid steel, slags and solid oxide solutions, for large numbers of components, have been developed over the last two decades by critical evaluation/optimization of all available phase equilibrium and thermodynamic data. The databases contain parameters of models specifically developed for molten slags; liquid and solid steel; and solid oxide solutions such as spinels. With user friendly software, which accesses these databases, complex equilibria involving slag, steel, inclusions, refractories and gases simultaneously, can be calculated for systems with many components, over wide ranges of temperature, oxygen potential and pressure. In the present article, several case studies will be presented, illustrating applications to complex steelmaking processes such as: Ca injection processes (Fe-Ca-Al-O inclusion diagram), corrosion of refractories, Mn/Si deoxidation, Ti/Al deoxidation (Fe-Al-Ti-O inclusion diagram), spinel formation (Fe-Mg-Al-O inclusion diagram), (Ti, N)(N, C) inclusion formation, oxide metallurgy.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Computer Applications of Thermodynamic Databases to Inclusion Engineering

twitter
facebook
mendeley

Bibtex

Ris

Numerical Investigation on Role of Bottom Gas Stirring in Controlling Thermal Stratification in Steel Ladles

Suvankar Ganguly, Suman Chakraborty

pp. 537-546

DOI:

10.2355/isijinternational.44.537

Abstract

A two dimensional Computational Fluid Dynamics (CFD) model was developed to simulate the fluid flow and heat transfer of the molten steel in a ladle during the holding time, with gas purging from the bottom. Transient analysis of the temperature and the velocity distribution of the liquid steel during ladle standing and subsequent gas stirring was conducted, by employing a pressure-based fully-implicit finite volume approach. Stratification, which can adversely affect the quality of steel products, was seen to develop due to natural convection. Therefore, particular attention was paid to study the effect of bottom gas stirring in minimizing the thermal stratification. This was accomplished by introducing a novel approach of coupling the effects of natural convection and axisymmetric bottom gas injection. Various parametric studies was undertaken to examine the effects of standing time, gas flow rate and geometry of the ladle on the resultant thermal field. It was observed that bottom purging situation induces a strong recirculatory flow in the molten steel bath, with an increase in the order of turbulence giving rise to thermal homogenization. The results indicate that the thermal stratification can be effectively eliminated by a relatively gentle agitation. Homogenization takes place at a faster rate with an increase in the amount of bottom gas flow. The effect of ladle size was found to be inconsequential, in comparison to other parameters.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Numerical Investigation on Role of Bottom Gas Stirring in Controlling Thermal Stratification in Steel Ladles

twitter
facebook
mendeley

Bibtex

Ris

Analysis on Refinement of Columnar γ Grain by Phosphorus in Continuously Cast 0.1 mass% Carbon Steel

Naotsugu Yoshida, Osamu Umezawa, Kotobu Nagai

pp. 547-555

DOI:

10.2355/isijinternational.44.547

Abstract

Based on a grain growth model, this paper discusses the γ grain refinement by phosphorus (P) in as cast 0.1 mass% C slabs. Two important factors, the starting temperature of the rapid grain growth (Trg) and the grain growth rate, are especially focused in the model. Local Equilibrium Mapping (LEM), an analytical method with local equilibrium calculations in the micro-segregation maps determined by EPMA, is carried out to evaluate the local transformation temperature and the γ phase fraction. The LEM analysis shows that the micro-segregation of P extends the δ/γ transformation temperature range to a lower temperature and retains the δ phase at a lower temperature. The Classical Grain Growth Model (CGM) based on a theory by Burke (1949) and Turnbull (1951) is derived, which assumes a normal grain growth with a parabolic law. The CGM successfully evaluates the γ grain growth curve in the as cast 0.1 mass% carbon steels considering the rapid growth after the δ/γ transformation and the change of the growth rate during cooling. The CGM analysis predicts the decrease of both Trg and growth rate by the P addition. The decrease of Trg was determined to be 160-170 K and agrees with the extension of the δ/γ transformation temperature range evaluated by the LEM analysis. Hence, the grain growth curves can be predicted by considering the extension of the δ/γ transformation temperature range due to the P addition and its micro-segregation.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Analysis on Refinement of Columnar γ Grain by Phosphorus in Continuously Cast 0.1 mass% Carbon Steel

twitter
facebook
mendeley

Bibtex

Ris

Numerical Simulation of Molten Steel Flow under a Magnetic Field with Argon Gas Bubbling in a Continuous Casting Mold

Noriko Kubo, Toshio Ishii, Jun Kubota, Toru Ikagawa

pp. 556-564

DOI:

10.2355/isijinternational.44.556

Abstract

In a continuous casting process, it is essential to prevent the surface defects which are caused by the entrapments of both mold powder and argon gas bubbles. It is well known through experiments that the decrease in the molten steel flow velocity just under the free surface is one of the most effective methods for the prevention of mold powder entrapments. For this purpose, we have already employed the electromagnetic force by the ElectroMagnetic Level Stabilizer (EMLS) system, which applies a low frequency alternating magnetic field that moves from the narrow face of the mold to the mold center below the nozzle exits. In this study, the molten steel flow in a mold was numerically analyzed to optimize the conditions for the prevention of the deteriorating phenomena: optimization of electromagnetic force with argon gas bubbling.
Simulation results indicate that argon gas bubbles ascend near the nozzle due to their buoyancy, and ascending argon bubbles induce the upstream of the molten steel. Due to the electromagnetic force, the molten steel is forced to flow toward the magnetic field traveling direction in the region where the magnetic field is imposed. Consequently, the molten steel flows toward the mold center near the free surface with a smaller imposed magnetic field, and it flows toward the narrow face with a larger imposed magnetic filed. A suitable imposed magnetic filed with argon gas bubbling can be chosen to minimize the flow velocity and also the amount of mold powder entrapments.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Numerical Simulation of Molten Steel Flow under a Magnetic Field with Argon Gas Bubbling in a Continuous Casting Mold

twitter
facebook
mendeley

Bibtex

Ris

Concentric Solidification for High Temperature Laser Scanning Confocal Microscopy

Mark Reid, Dominic Phelan, Rian Dippenaar

pp. 565-572

DOI:

10.2355/isijinternational.44.565

Abstract

A new experimental technique defined as concentric solidification has been developed to improve in-situ observations of solidification and high temperature phase transformations using laser scanning confocal microscopy (LSCM). The technique consists of applying a radial thermal gradient across a 10 mm diameter sample such that the maximum temperature is focused in the centre of the specimen. Careful control over the sample thickness, heating rate and peak temperature results in the formation of a liquid pool in the centre of the specimen. Surface tension balance between solid, liquid, gas and crucible result in minimal meniscus formation on the liquid pool, leading to a greatly enhanced in-situ observations. Examples of the range of observations possible as well as unique observations of segregation related phenomena are presented.

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Concentric Solidification for High Temperature Laser Scanning Confocal Microscopy

twitter
facebook
mendeley

Bibtex

Ris

Blast Furnace Hot Metal Temperature Prediction through Neural Networks-Based Models

Juan Jiménez, Javier Mochón, Jesús Sainz de Ayala, Faustino Obeso

pp. 573-580

DOI:

10.2355/isijinternational.44.573

Abstract

Blast furnace hot metal temperature prediction, by mean of mathematical models, plays an interesting role in blast furnace control, helping plant operators to give a faster and more accurate answer to changes in blast furnace state. In this work, the development of parametric models based on neural networks is shown. Time has been included as an implicit variable to improve consistency. The model has been developed departing from actual plant data supplied by Aceralia from its steel works located in Gijón.

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Blast Furnace Hot Metal Temperature Prediction through Neural Networks-Based Models

twitter
facebook
mendeley

Bibtex

Ris

Creep Behavior of 2.25Cr-1Mo Steel Shield Metal Arc Weldment

Shimpei Fujibayashi, Koji Kawano, Takayuki Komamura, Takaya Sugimura

pp. 581-590

DOI:

10.2355/isijinternational.44.581

Abstract

In order to guarantee the safety of high temperature components and prevent unscheduled outage, remnant life assessment for creep is quite important. The experiences in actual components reveal that almost all the problems relating to creep are generated at the weldment, which contains microstructures with different creep properties from those presumed in the parent material. Nowadays, it is generally accepted that a terminal failure mode of low alloy ferritic steels or tempered martensitic steels become Type IV, taking place at the Intercritical HAZ or Fine Grained HAZ. However, in the present work using 2.25Cr-1Mo steel welds fabricated with basic coated Shield Metal Arc Weld (SMAW) consumables, the most prevalent failure mode was Type I in the center of weld metal rather than Type IV. And this tendency was more pronounced at low stresses, suggesting the possibility of Type I cracking in actual components. It was concluded that poor creep strength of 2.25Cr-1Mo weld metal was ascribed to its fully bainitic microstructure in which carbides evolution was accelerated and M2C depletion took place earlier than base metal.

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Creep Behavior of 2.25Cr-1Mo Steel Shield Metal Arc Weldment

twitter
facebook
mendeley

Bibtex

Ris

Effect of the Hot Band Grain Size and Intermediate Annealing on the Deformation and Recrystallization Textures in Low Silicon Electrical Steels

Marcos F. de Campos, Fernando J. G. Landgraf, Rubens Takanohashi, Fabio C. Chagas, Ivan G. S. Falleiros, Gabriela C. Fronzaglia, Henrique Kahn

pp. 591-597

DOI:

10.2355/isijinternational.44.591

Abstract

The effect of hot band grain size on the texture of low silicon steels was investigated. In spite of different hot band grain sizes (22, 125 and 500 μm), the deformation texture is formed by the fibers ‹111›//ND and ‹110›//RD. Nevertheless the recrystallization texture is strongly affected. Increasing the hot band grain size, from 22 to 125 μm, the intensity of the Goss component in the recrystallized material increases and {111} components decreases. The further increase to 500 μm does not increase Goss, but increases cube on face component. When the hot band grain size is sufficiently large (500 μm) the deformed grains tend to recrystallize independently, originating regions (clusters) of grains with same orientation. There is no apparent effect of an intermediate recovery (after deformation ε=0.7 annealing at 500°C during 1 h) on the deformation or recrystallization textures.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Effect of the Hot Band Grain Size and Intermediate Annealing on the Deformation and Recrystallization Textures in Low Silicon Electrical Steels

twitter
facebook
mendeley

Bibtex

Ris

Improvement of Cutting Tool Life by AlN Deposition on the Tool

Hiroshi Yaguchi, Katsuhiko Ozaki, Masami Somekawa

pp. 598-602

DOI:

10.2355/isijinternational.44.598

Abstract

SCM415 steel was machined with carbide tools in as hot rolled condition and after normalizing heat treatment. In the as-rolled sample, a significant amount of Al and N existed as solid solution; whereas, in the normalized sample, Al and N existed as AlN precipitates. Reduction of tool wear for the as-rolled sample was observed. On the rake face of the tool machined for the as-rolled sample, the presence of AlN deposit was observed. It is believed that Al and N in solid solution form AlN deposit on the tool face due to temperature rise during machining, and that the deposition of the AlN layer on the tool face prevents diffusion between the tool and chip and reduces tool wear.

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Improvement of Cutting Tool Life by AlN Deposition on the Tool

twitter
facebook
mendeley

Bibtex

Ris

Effects of Microstructure on Stretch-flange-formability of 980 MPa Grade Cold-rolled Ultra High Strength Steel Sheets

Kohei Hasegawa, Kenji Kawamura, Toshiaki Urabe, Yoshihiro Hosoya

pp. 603-609

DOI:

10.2355/isijinternational.44.603

Abstract

Stretch-flange-formability is an important property for ultra high strength steel (UHSS) sheets for press-forming. In this study, microscopic deformation behaviors during punching and following stretch-flange-forming were investigated using three types of 980 MPa grade UHSS sheets with either two ferrite/martensite dual-phase structures or a martensite single-phase structure in order to clarify how the microstructure affects the stretch-flange-formability of UHSS sheets. The results of this investigation revealed following conclusions. Microscopic plastic-flow or micro-void density generated by punching is not the dominant factor of the stretch-flange-formability of UHSS sheets. During hole-expanding, cracks were mainly initiated at the fractured surface part and the cracks became longer and deeper from the punched surface with the increase of hole-expanding ratio. Deep cracking resistance in this process is important to improve the stretch-flange-formability. The existence of strain gradient induced by hole punching is considered to be one of the reason for the highest hole-expanding ratio of the martensite single phase steel. During hole-expanding, the micro-cracks propagate mostly along the phase interfaces in the dual-phase steel sheets in the case of poor stretch-flange-formability, while the micro-cracks are tend to propagate through ferrite and martensite phases in the case of high stretch-flange-formability. The analysis of the hardness of ferrite and martensite suggests that the difference in hardness is the dominant factor of the stretch-flange-formability of the dual-phase steel. In addition, the volume fractions of phases also influence the formability.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Effects of Microstructure on Stretch-flange-formability of 980 MPa Grade Cold-rolled Ultra High Strength Steel Sheets

twitter
facebook
mendeley

Bibtex

Ris

Ductile-Brittle Transition Temperature of Ultrafine Ferrite/Cementite Microstructure in a Low Carbon Steel Controlled by Effective Grain Size

T. Hanamura, F. Yin, K. Nagai

pp. 610-617

DOI:

10.2355/isijinternational.44.610

Abstract

To analyze the good toughness of ultrafine ferrite/cementite steels, the concept of effective grain size (dEFF) is applied to ductile-to-brittle transition temperature, DBTT, for ultrafine ferrite/cementite (Uf-F/C), ferrite/pearlite (F/P), quenched (Q), and quench-and-tempered (QT) microstructures in a low carbon steel. The dEFF is determined to be 8, 20, 100, and 25 μm for Uf-F/C, F/P, Q, and QT, respectively. In F/P and Q, it is in accordance with the ferrite grain size and the prior austenite grain size, respectively. In QT, the dEFF fits the martensite packet size. In Uf-F/C, the ferrite grain size has a bimodal distribution and the larger grain size corresponds to the dEFF, which is the smallest among the four microstructures. In terms of the relationship between dEFF and DBTT, the Uf-F/C, Q, and QT microstructures can be placed into the same group and the F/P to a different one. Furthermore, the Uf-F/C has the highest estimated fracture stress among the four microstructures. These might be the result of the difference in the surface energy of fracture, namely the former is estimated to have a surface energy of 34.6 J/m2 and latter a surface energy of 7.7 J/m2. Thus, the excellent toughness of the ultrafine ferrite/cementite steel can be attributed to the small dEFF and the high surface energy of fracture.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Ductile-Brittle Transition Temperature of Ultrafine Ferrite/Cementite Microstructure in a Low Carbon Steel Controlled by Effective Grain Size

twitter
facebook
mendeley

Bibtex

Ris

Decarburization Kinetics during Annealing of a Semi-processed Electrical Steel

Kleiner Marques Marra, Evandro de Azevedo Alvarenga, Vicente Tadeu Lopes Buono

pp. 618-622

DOI:

10.2355/isijinternational.44.618

Abstract

Semi-processed, non-oriented electrical steels used in motor and transformer cores have their magnetic properties optimized by means of a heat treatment performed under a moistened nitrogen atmosphere containing small amounts of hydrogen. The oxidation of carbon on the steel surface by the oxidizing gases present in this atmosphere decreases the carbon content of the steel. The consequent reduction in the amount of soluble carbon and in the volume fraction of carbides reduces magnetic losses and the susceptibility of the steel to magnetic aging. In this work, a cold-rolled, semi-processed electrical steel was submitted to six thermal treatments covering the most usual conditions employed in industry, combining two types of atmosphere (mixtures of nitrogen with 5% and 10% H2) and three dew points (10, 20 and 30°C). The treatments were carried out in a pilot electrical oven especially adapted to simulate the thermal cycle and the moistened atmospheres employed in industry. The results obtained show that, at the beginning of the process, the decarburization rate is controlled by the chemical reaction of carbon on the steel surface. Later, an oxide layer may build up, depending on the humidity level of the atmosphere, reducing the rate of decarburization.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Decarburization Kinetics during Annealing of a Semi-processed Electrical Steel

twitter
facebook
mendeley

Bibtex

Ris

Dissolution Mechanism of Fluorine in Aqueous Solution from Fluorine Containing Synthetic Slag

Hideo Mizukami, Minoru Ishikawa, Takeyuki Hirata, Takanori Kamiyama, Kenji Ichikawa

pp. 623-629

DOI:

10.2355/isijinternational.44.623

Abstract

The behavior of dissolution of fluorine from the fluorine containing synthetic slag was clarified by the shaking test under various experimental conditions. The fluorine containing minerals were cuspidine, fluorapatite and fluorite. The amount of fluorine dissolved from the slag increased with an increasing of the concentration of fluorine in the slag and an decreasing of the size of slag particles. The amount of fluorine dissolved from the slag could be estimated from the size distribution of slag particle and the concentration of slag for the shaking test. The amount of fluorine dissolved from the slag decreased with an increasing of the basicity of slag and the concentration of alumina. The amount of fluorine from the slag increased with increasing the cooling rate during solidification because the slag became amorphous. The dissolution of fluorine from the slag was controlled by the mass transfer in the liquid layer which was formed near the surface of slag.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Dissolution Mechanism of Fluorine in Aqueous Solution from Fluorine Containing Synthetic Slag

twitter
facebook
mendeley

Bibtex

Ris

Immobilization Mechanism of Fluorine in Aqueous Solution from Road Material Containing Synthetic Hot Metal Pretreatment Slag by Shaking Test

Hideo Mizukami, Minoru Ishikawa, Takeyuki Hirata, Takanori Kamiyama, Kenji Ichikawa

pp. 630-635

DOI:

10.2355/isijinternational.44.630

Abstract

The ability of immobilization of fluorine dissolved from the fluorine containing slag with the calcium compound was evaluated by the shaking test. In the calcium compounds which have the ability of immobilization of fluorine, the 12CaO · 7Al2O3 was found to be the largest ability. From the results of evaluating the stability of immobilization with 12CaO · 7Al2O3, it was shown that the dissolved fluorine from slag was immobilized for 100 h in shaking time. It was confirmed from the experimental results of X-ray analysis and the equilibrium thermodynamic calculation for aqueous solution that the generation of fluorite which was hard to dissolve in aqueous solution enabled the immobilization of fluorine dissolved from slag. Moreover, the 12CaO · 7Al2O3 of 5-15 mass% could be used for the road construction material which consisted of fluorine containing slag and blast furnace slag and as a result the immobilization of fluorine was confirmed.

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Immobilization Mechanism of Fluorine in Aqueous Solution from Road Material Containing Synthetic Hot Metal Pretreatment Slag by Shaking Test

twitter
facebook
mendeley

Bibtex

Ris

Spout Eye Area in Ladle Refining Process

Manabu Iguchi, Ken-ichiro Miyamoto, Shintaro Yamashita, Daisuke Iguchi, Masafumi Zeze

pp. 636-638

DOI:

10.2355/isijinternational.44.636

Readers Who Read This Article Also Read

mendeley

Bookmark

Detail

PDF Download

Share it with SNS

Article Title

Spout Eye Area in Ladle Refining Process

twitter
facebook
mendeley

Bibtex

Ris

Article Access Ranking

21 Nov. (Last 30 Days)

You can use this feature after you logged into the site.
Please click the button below.

Advanced Search

Article Title

Author

Abstract

Journal Title

Year

Please enter the publication date
with Christian era
(4 digits).

Please enter your search criteria.