Quantifying the origin of metallic glass formation

被引:151
作者
Johnson, W. L. [1 ]
Na, J. H. [2 ]
Demetriou, M. D. [1 ,2 ]
机构
[1] 138 78 Calif Inst Technol, Dept Mat Sci, Keck Lab Engn, Pasadena, CA 91125 USA
[2] Glassimet Technol Inc, 2670 Walnut St Ave, Pasadena, CA 91107 USA
关键词
SUPERCOOLED LIQUID; COOLING RATE; NUCLEATION; ALLOYS; TEMPERATURE; TRANSITION; LANDSCAPE; VISCOSITY; RHEOLOGY;
D O I
10.1038/ncomms10313
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
The waiting time to form a crystal in a unit volume of homogeneous undercooled liquid exhibits a pronounced minimum tau(star)(X) at a 'nose temperature' T-star located between the glass transition temperature T-g, and the crystal melting temperature, T-L. Turnbull argued that tau X-star should increase rapidly with the dimensionless ratio t(rg) = T-g/T-L. Angell introduced a dimensionless 'fragility parameter', m, to characterize the fall of atomic mobility with temperature above Tg. Both t(rg) and m are widely thought to play a significant role in determining tau(star)(X). Here we survey and assess reported data for T-L, T-g, t(rg), m and tau X star for a broad range of metallic glasses with widely varying tau(X)star. By analysing this database, we derive a simple empirical expression for tau(star)(X)(t(rg), m) that depends exponentially on t(rg) and m, and two fitting parameters. A statistical analysis shows that knowledge of t(rg) and m alone is therefore sufficient to predict tau(star)(X) within estimated experimental errors. Surprisingly, the liquid/crystal interfacial free energy does not appear in this expression for tau(star)(X).
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页数:7
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