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Erschienen in: Metallurgical and Materials Transactions A 10/2014

01.09.2014

The Strength of the Spatially Interconnected Eutectic Network in HPDC Mg-La, Mg-Nd, and Mg-La-Nd Alloys

verfasst von: Bao Zhang, Serge Gavras, Anumalasetty V. Nagasekhar, Carlos Horacio Cáceres, Mark A. Easton

Erschienen in: Metallurgical and Materials Transactions A | Ausgabe 10/2014

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Abstract

3D numerical images of the intergranular percolating eutectic of two binary alloys, Mg-0.62 at. pctLa and Mg-0.60 at. pctNd, created using dual beam FIB tomography, were incorporated into an FEM code to model their tensile behavior. Due to its high volume fraction (29.9 pct), the behavior of the Mg-La network was akin to that of a stretch-dominated micro-truss structure, whereas the Mg-Nd’s, with a relatively low volume fraction (7.5 pct), mimicked that of a bending-dominated structure. The 3D network contributed some 37 MPa to the strength of the Mg-La alloy casting, whereas it only added about 1.4 MPa to the Mg-Nd’s. The model predictions based on the binary alloys were verified using cast-to-shape specimens of the Mg-La and two ternary Mg-La-Nd alloys, subjected to a flash-annealing aiming at breaking up the continuity of the 3D network, while preserving the rest of the microstructure unchanged. The flash-annealed specimens exhibited a decrease in strength that matched closely the computed values. Implications regarding alloy design involving the eutectic network and solid solution hardening of more complex alloys are discussed.

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Fußnoten
1
Similar modeling[9] for alloy AZ91D showed that varying the Poisson’s ratio within the range bounded by the values for the pure Mg and that of the intermetallic has negligible effects on the calculated stress–strain behavior of the percolating structure.
 
2
In Reference 9 the intermetallic network of alloy AZ91D was considered under a compressive stress in the undeformed alloy due to the difference in the coefficient of thermal expansion (CTE) between Mg matrix and the intermetallic. In the present case, the intermetallic and surrounding eutectic α-Mg are considered as a unit, and any internal stresses arising from thermal effects between the two components were assumed to balance out.
 
3
In comparison with the Voigt’s bound, which assumes all micro-trusses aligned parallel to the stress axis, in the SD configuration only 1/3 of the interconnected branches are loaded in tension, with the rest orientated across the tensile axis. In the BD configuration loads are transmitted exclusively through elastic bending of the micro-trusses.[24]
 
4
For ε < 0.7 pct, the strain hardening rate reflects the rapid development of a back stress due to the formation of dislocation pile ups on the obstacles to primary micro-slip, whereas for ε > 0.7 pct, linear hardening is observed due to the steady accumulation of forest dislocations when full plasticity develops.[17,25,33]
 
5
The increase in ductility of the flash-annealed specimens is not as large as it might be expected from Fig. 5. Possible factors to invoke are the cracking of the intermetallic overloaded by dispersion hardening effects, and the presence of microporosity, which can have an overriding effect on the tensile ductility.
 
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Metadaten
Titel
The Strength of the Spatially Interconnected Eutectic Network in HPDC Mg-La, Mg-Nd, and Mg-La-Nd Alloys
verfasst von
Bao Zhang
Serge Gavras
Anumalasetty V. Nagasekhar
Carlos Horacio Cáceres
Mark A. Easton
Publikationsdatum
01.09.2014
Verlag
Springer US
Erschienen in
Metallurgical and Materials Transactions A / Ausgabe 10/2014
Print ISSN: 1073-5623
Elektronische ISSN: 1543-1940
DOI
https://doi.org/10.1007/s11661-014-2416-9

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