Effect of Interfacial Energy on Distribution of Nanoparticle in the Melt During the Preparation of Fe-Based ODS Alloys by Thermite Reaction
Jianxue LIU, Wenjun XI(), Neng LI, Shujie LI
School of Materials Science and Engineering, Beihang University, Beijing 100191, China
Cite this article:
Jianxue LIU, Wenjun XI, Neng LI, Shujie LI. Effect of Interfacial Energy on Distribution of Nanoparticle in the Melt During the Preparation of Fe-Based ODS Alloys by Thermite Reaction. Acta Metall Sin, 2017, 53(8): 1011-1017.
Fe-based oxide dispersion strengthened (ODS) alloys are conventionally manufactured through mechanical alloying. Such route even involves an expensive milling step but the oxide surface still could not avoid being contaminated. This work developed a new method by combination of thermite reaction and rapid solidification (RS) to prepare ODS alloys. Attributing to the optimization of thermite mixture composition, nanoparticle α-Al2O3 was synthetized in situ and the molten alloy was modulated by spinodal decomposition (SD) into Fe, Cr-rich and Ni, Al-rich regions. During the cooling of the melt, the low interfacial energy between α-Al2O3 and Ni, Al-rich region was also considered in the process for nanoparticles α-Al2O3 to assemble into NiAl, thus they could uniformly distribute in matrix. This work focuses on the thermodynamic analysis of SD in the melt alloy and the speed of the nanoparticles α-Al2O3 under the influence of interfacial energy and Brownian motion. Experiment results shows that the spherical NiAl segregated by SD has a mean diameter of about 50 nm, whose volume fraction reaches up to 50%; and nanoparticle α-Al2O3, formed during thermite reaction, has a diameter of 5 nm combined into NiAl under the influence of interfacial energy. Computation results indicate that, driven by interfacial energy and Brownian motion, nanoparticle α-Al2O3 could move fast enough into Ni, Al-rich region before solidification accomplishes during RS. Test results imply that the tensile strength of Fe-based ODS alloy is 602 MPa with ultimate elongation of 21% and its mass gain under 1000 ℃ in air for 100 h is 0.4 mg/cm2.
Fig.2 XRD spectrum of Fe-based oxide dispersion strengthened (ODS) alloy synthesized by thermite reaction process
Fig.3 Low (a) and high (b) magnified TEM images, HRTEM image (c) and SAED pattern (d) of Fe-based ODS alloys synthesized by thermite reaction process
Fig.4 Schematic of simplified motion diagram of nanoparticle Al2O3
Material
Yield strength
Ultimate tensile
ultimate
Mass gain
Ref.
MPa
strength / MPa
elongation / %
mgcm-2
MA956
493
591
28.5
0.3
[32, 33]
PM2000
870
890
13
0.4
[34~36]
MA754 (Ni-based)
688
1052
23
0.8
[37, 38]
Fe-based ODS alloy
394
602
21
0.4
This work
Table 1 Tensile strength and mass gain after oxidation of Fe-based ODS alloy synthesized by thermite reaction process with respect to some commercial ODS alloys
[1]
Wright I G, Wilcox B A, Jaffee R I.The high-temperature oxidation of Ni-20%Cr alloys containing various oxide dispersions[J]. Oxid. Met., 1975, 9: 275
[2]
Nagai H, Takebayashi Y, Mitani H.Effect of dispersed oxides of rare earths and other reactive elements on the high temperature oxidation resistance of Fe-20Cr alloy[J]. Metall. Trans., 1981, 12A: 435
[3]
Ukai S, Harada M, Okada H, et al.Alloying design of oxide dispersion strengthened ferritic steel for long life FBRs core materials[J]. J. Nucl. Mater., 1993, 204: 65
[4]
Merzhanov A G.Self-propagating high-temperature synthesis: twenty years of search and findings [A]. Combustion and Plasma Synthesis of High-Temperature Materials[M]. New York: VCH Publishers, 1990: 1
[5]
Duan H P, Sheng Y, Liu M, et al.Stainless steel lined composite steel pipe produced by centrifugal SHS process[J]. J. Mater. Sci. Lett., 1996, 15: 1060
[6]
Xi W J, Yin S, Guo S J, et al.Stainless steel lined composite steel pipe prepared by centrifugal-SHS process[J]. J. Mater. Sci., 2000, 35: 45
[7]
Xi W J, Peng R L, Wu W, et al.Al2O3 nanoparticle reinforced Fe-based alloys synthesized by thermite reaction[J]. J. Mater. Sci., 2012, 47: 3585
[8]
Cui Y, Xi W J, Wang X, et al.Al2O3 nanoparticle and NiAl reinforced Fe-based ODS alloys synthesized by thermite reaction[J]. Acta Metall. Sin., 2015, 51: 791(崔跃, 席文君, 王星等. 纳米Al2O3和NiAl共同强化的铁基ODS合金的铝热合成研究[J]. 金属学报, 2015, 51: 791)
[9]
Wang X, Xi W J, Cui Y, et al.Microstructure evolution mechanism and mechanical properties of FeNiCrAl alloy reinforced by coherent NiAl synthe-sized by thermite process[J]. Acta Metall. Sin. 2015, 51: 483(王星, 席文君, 崔跃等. 铝热合成NiAl共格强化的FeNiCrAl合金的组织演化机理和力学性能[J]. 金属学报, 2015, 51: 483)
[10]
Wu W, Xi W J.Effect of heat decomposition process and thermal treatment for TiO2 Xerogel powder on surface organic functional groups[J]. Chin. J. Inorg. Chem., 2011, 27: 659(吴伟, 席文君. 二氧化钛干凝胶热分解及热处理对表面有机官能团变化的影响[J]. 无机化学学报, 2011, 27: 659)
[11]
Chen R F, Liu H T.Preparation of Cr-doped TiO2/SiO2 photocatalysts and their photocatalytic properties[J]. J. Chin. Chem. Soc., 2011, 58: 947
[12]
Hao S M, Ishida K, Nishizawa T.Role of alloying elements in phase decomposition in alnico magnet alloys[J]. Metall. Trans., 1985, 16A: 179
[13]
Bradley A J.Microscopical studies on the iron-nickel-aluminium system. Part I——α+β alloys and isothermal sections of the phase equilibrium diagram[J]. J. Iron Steel Inst., 1949, 163: 19
[14]
Bradley A J.Microscopical studies on the iron-nickel-aluminium system. Part II——The breakdown of the body-centered cubic lattice[J]. J. Iron Steel Inst., 1951, 168: 233
[15]
Bradley A J.Microscopical studies on the iron-nickel-aluminium system. Part III——Transformations of the β and β' phase[J]. J. Iron Steel Inst., 1952, 171: 41
[16]
Hao S M, Takayama T, Ishida K, et al.Miscibility gap in Fe-Ni-Al and Fe-Ni-Al-Co systems[J]. Metall. Trans., 1984, 15A: 1819
[17]
Wang C P, Liu X J, Ohnuma I, et al.Thermodynamic database of the phase diagrams in Cu-Fe base ternary systems[J]. J. Phase Equilib. Diff., 2004, 25: 320
[18]
Baumli P, Sytchev J, Kaptay G.Perfect wettability of carbon by liquid aluminum achieved by a multifunctional flux[J]. J. Mater. Sci., 2010, 45: 5177
[19]
Rohrer G S.Grain boundary energy anisotropy: A review[J]. J. Mater. Sci., 2011, 46: 5881
[20]
Triantafyllou G, Angelopoulos G N, Nikolopoulos P.Surface and grain-boundary energies as well as surface mass transport in polycrystalline yttrium oxide[J]. J. Mater. Sci., 2010, 45: 2015
[21]
Nikolopoulos P, Agathopoulos S, Tsoga A.A method for the calculation of interfacial energies in Al2O3 and ZrO2/liquid-metal and liquid-alloy systems[J]. J. Mater. Sci., 1994, 29: 4393
[22]
Sharan A, Cramb A W.Surface tension and wettability studies of liquid Fe-Ni-O alloys[J]. Metall. Mater. Trans., 1997, 28B: 465
[23]
Silvain J F, Bihr J C, Douin J.Wettability, reactivity and stress relaxation of an NiAl(Ti)/Al2O3 composite[J]. Compos. Appl. Sci. Manuf., 1998, 29A: 1175
[24]
Nakanishi K, Soga N.Phase separation in silica sol-gel system containing polyacrylic acid I. Gel formaation behavior and effect of solvent composition[J]. J. Non-Cryst. Solids, 1992, 139: 1
[25]
Kaptay G.Interfacial criterion of spontaneous and forced engulfment of reinforcing particles by an advancing solid/liquid interface[J]. Metall. Mater. Trans., 2001, 32A: 993
[26]
K?rber C, Rau G, Cosman M D, et al.Interaction of particles and a moving ice-liquid interface[J]. J. Cryst. Growth, 1985, 72: 649
[27]
Uhlmann D R, Chalmers B, Jackson K A.Interaction between particles and a solid-liquid interface[J]. J. Appl. Phys., 1964, 35: 2986
[28]
Sen S, Dhindaw B K, Stefanescu D M, et al.Melt convection effects on the critical velocity of particle engulfment[J]. J. Cryst. Growth, 1997, 173: 574
[29]
Washizu T, Nagasaka T, Hino M.Viscosity of liquid Fe-Cu-Si alloy formed in new melting process for domestic waste incineration residue[J]. Mater. Trans., 2001, 42: 471
[30]
Huang Z Q, Ding E J.Surface Wetting and Wetting Transition [M]. Shanghai: Shanghai Science & Technical Publishers, 1994: 40(黄祖洽, 丁鄂江. 表面浸润和浸润相变 [M]. 上海: 上海科学技术出版社, 1994: 40)
[31]
Chen Z Q, Dai M G.Colloidal Chemistry [M]. Beijing: Higher Education Press, 1984: 38(陈宗淇, 戴闽光. 胶体化学[M]. 北京: 高等教育出版社, 1984: 38)
[32]
Wang J Y, Yuan W, Mishra R S, et al.Microstructure and mechanical properties of friction stir welded oxide dispersion strengthened alloy[J]. J. Nucl. Mater., 2013, 432: 274
[33]
Quadakkers W J, Holzbrecher H, Briefs K G, et al.Differences in growth mechanisms of oxide scales formed on ODS and conventional wrought alloys[J]. Oxid. Met., 1989, 32: 67
[34]
Klueh R L, Shingledecker J P, Swindeman R W, et al.Oxide dispersion-strengthened steels: a comparison of some commercial and experimental alloys[J]. J. Nucl. Mater., 2005, 341: 103
[35]
Montealegre M A, Strehl G, González-Carrasco J L, et al. Oxidation behaviour of novel ODS FeAlCr intermetallic alloys[J]. Intermetallics, 2005, 13: 896
[36]
Weinbruch S, Anastassiadis A, Ortner H M, et al.On the mechanism of high-temperature oxidation of ODS superalloys: significance of yttrium depletion within the oxide scales[J]. Oxid. Met., 1999, 51: 111
[37]
Wittenberger J D.Creep and tensile properties of several oxide-dispersion-strengthened nickel-base alloys at 1365 K [R]. Cleveland, OH, United States: NASA Lewis Research Center, 1977
[38]
Pint B A, Wright I G.Oxidation behavior of ODS Fe-Cr alloys[J]. Oxid. Met., 2005, 63: 193
[39]
Sokolov M A, Hoelzer D T, Stoller R E, et al. Fracture toughness and tensile properties of nano-structured ferritic steel 12YWT [J]. J. Nucl. Mater., 2007, 367-370: 213