Research Articles

Induced solidification of liquid Al from molecular dynamics simulation

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  • State Key Laboratory of Advanced Special Steel, Shanghai Key Laboratory of Advanced Ferrometallurgy, School of Materials Science and Engineering, Shanghai University, Shanghai 200444, China

Received date: 2018-04-13

  Online published: 2018-12-21

Abstract

Molecular dynamics (MD) simulation was applied to analyze the solidification of liquid Al induced by embedded solid nanoparticles with radii ranging from 0.37 to 2.4 nm. It was found that the critical temperature was proportional to the inverse of the nucleus radius, i.e., Gibbs-Thomson (G-T) effect, through which the G-T coefficient Γ and the bulk melting temperature Tmbulk were obtained, 1.41.4*10-7 Km and (985.36±11.25) K, respectively. The solid-liquid interfacial energy which was estimated (140.35±9.05)mJ/m2 from Γ, was very close to the calculated 149 mJ/m2 by capillary fluctuation method. It proved again that Turnbull underestimated this quantity experimentally (93 mJ/m2). The critical failure radius was extrapolated to be 0.91 nm. Meanwhile, the corresponding system temperature had reached the lower limit for the critical temperature, under which the system could be spontaneously nucleated, and the incubation time was somewhat random. Besides, the microstructure was characterized by the metastable cross stacking faults. When the embedded nucleus could serve as the nucleation core, the incubation time increased with increasing embedded nucleus radius. However, the growth rate decreased separately with the increasing embedded nucleus radius. The microstructure adopted the relatively stable lamellar structure.

Cite this article

YU Ronggang, LAI Qinmei, WANG Hao, WU Yongquan . Induced solidification of liquid Al from molecular dynamics simulation[J]. Journal of Shanghai University, 2020 , 26(2) : 216 -226 . DOI: 10.12066/j.issn.1007-2861.2038

References

[1] Turnbull D . Formation of crystal nuclei in liquid metals[J]. Journal of Applied Physics, 1950,21(10):1022-1028.
[2] Espinosa J R, Vega C, Valeriani C , et al. Seeding approach tocrystal nucleation[J]. Journal of Chemical Physics, 2016,144(3):1-10.
[3] Bai X M, Li M . Calculation of solid-liquid interfacial freeenergy: a classical nucleation theory based approach[J]. Journal ofChemical Physics, 2006,124(12):1-12.
[4] Broughton J Q, Gilmer G H . Molecular dynamics investigation ofthe crystal-fluid interface. VI. Excess surface free energies ofcrystal-liquid systems[J]. Journal of Chemical Physics, 1986,84(10):5759-5768.
[5] Hoyt J J, Asta M, Karma A . Method for computing the anisotropyof the solid-liquid interfacial free energy[J]. Physical ReviewLetters, 2001,86(24):5530-5533.
[6] Shibuta Y, Suzuki T . A molecular dynamics study of the phasetransition in BCC metal nanoparticles[J]. Journal of ChemicalPhysics, 2008,129(14):1-10.
[7] Watanbe Y, Shibuta Y, Suzuki T . A molecular dynamics study ofthermodynamic and kinetic properties of solid-liquid interface forBCC iron[J]. ISIJ International, 2010,50(8):1158-1164.
[8] Hashimoto R, Shibuta Y, Suzuki T . Estimation of solid-liquidinterfacial energy from Gibbs-Thomson effect: a molecular dynamicsstudy[J]. ISIJ International, 2011,51(10):1664-1667.
[9] Xia Y, Li C H, Luan Y W , et al. Molecular dynamics studies onthe correlation of undercoolability and thermophysical properties ofliquid Ni-Al alloys[J]. Computational Materials Science, 2016,1112(1):383-394.
[10] Wu Y Q, Shen T, Lu X M , et al. Solidification of liquid Fe withembedded homogeneous solid Fe nanoparticles from molecular dynamicssimulations[J]. Acta Physico-Chimica Sinica, 2013,29(2):245-249.
[11] Plimpton S . Fast parallel algorithms for short-range moleculardynamics[J]. Journal of Computational Physics, 1995,117(1):1-19.
[12] Mendelev M I, Han S, Srojovitz D J , et al. Development of newinteratomic potentials appropriate for crystalline and liquid iron[J]. Philosophical Magazine, 2003,83(35):3977-3994.
[13] Jiang Y W, Luo J, Wu Y Q . The validation and preference amongdifferent EAM potentials to describe the solid-liquid transition ofaluminum[J]. Modelling and Simulation in Materials Science andEngineering, 2017,25(4):1-13.
[14] Li R, Wu Y Q, Xiao J J . The nucleation process and the roles ofstructure and density fluctuations in supercooled liquid Fe[J]. Journal of Chemical Physics, 2014,140(3):1-11.
[15] Zhou H G, Lin X, Wang M , et al. Calculation of crystal-meltinterfacial free energies of FCC metals[J]. Journal of CrystalGrowth, 2013,366(3):82-87.
[16] Liu J, Dong H B . Molecular dynamics calculation ofthermodynamic properties of iron solidification[J]. IOP ConferenceSeries: Materials Science and Engineering, 2012,33(1):1-10.
[17] Chase M W, Curnutt J L, Downey J R , et al. JANAF thermochemicaltables, 1982 supplement[J]. Journal of Physical and ChemicalReference Data, 1982,11(3):695-940.
[18] Kelton K F . Crystal nucleation in liquids and glasses[J]. Solid State Physics, 1991,45(1):75-177.
[19] Morris J R . Complete mapping of the anisotropic free energy ofthe crystal-melt interface in Al[J]. Physical Review B, 2002,66(14):1-7.
[20] Morris J R, Mendelev M I, Srojovitz D J . A comparison ofcrystal-melt interfacial free energies using different Al potentials[J]. Journal of Non-Crystalline Solids, 2007,353(32):3565-3569.
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