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COST 507 - Repositório Aberto da Universidade do Porto

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Thermodynamic Assessment in the Al­Cu­Mg­Zn System<br />

Dll<br />

P. Liang, H. L. Lukas, H. J. Seifert and F. Aldinger<br />

Max­Planck­Institut für Metallforschung, Pulvermetallurgisches Laboratorium,<br />

Heisenbergstr. 5, D­70569 Stuttgart, Germany<br />

Abstract<br />

The main part of this research is the assessment of the Al­Cu­Mg­Zn system, which<br />

is one of the key systems of the <strong>COST</strong> <strong>507</strong> project. Our contribution to it includes<br />

full optimization of the Cu­Mg­Zn and Al­Mg­Zn ternary systems and revision of the<br />

thermodynamic descriptions of the Ai­Mg, Mg­Si, Mg­Zn and Al­Mg­Si systems, using<br />

experimental results planned after the assessments of round I and carried out by<br />

our partners of the <strong>COST</strong> <strong>507</strong> project. The optimization of the Al­Mg­Zn ternary<br />

system incorporates, in addition to the available published <strong>da</strong>ta, the results of experimental<br />

measurements carried out in a collaboration between CNRS at Vitry­sur­Seine,<br />

UMIST Manchester and MPI Stuttgart. The experiments on ternary Al­Mg­Zn alloys<br />

were specifically performed to provide missing <strong>da</strong>ta of the ternary solubilities of the<br />

ΑΙ­Mg and Mg­Zn phases as well as to improve the knowledge of the extensions of the<br />

homogeneity ranges of the ternary r- and ^­phases.<br />

In the Al­Mg­Si system the technically most important part, the solvus surface of the<br />

(Al) solid solution could be improved, on one hand due to a better description of the<br />

Gibbs energy of the Mg2Si binary phase, derived from enthalpy of formation and melting<br />

as well as from heat capacity measurements, on the other hand by DTA, dilatometrie<br />

and metallographic investigation of Al­rich alloys, which were carried out by F. Sommer'<br />

s group at MPI Stuttgart.<br />

1 Introduction<br />

The phase relationships in the quaternary Al­Cu­Mg­Zn system are very complex and<br />

experimentally not well established. Only a partial phase diagram in the Al­rich corner<br />

was investigated [47Str]. No quaternary phase has been found. I. e. the phases encountered<br />

are the same as in the ternary sub­systems Al­Cu­Mg, Al­Cu­Zn, Al­Mg­Zn and<br />

Cu­Mg­Zn or quaternary extensions of them.<br />

In the Al­Cu­Mg­Zn system, several non­stoichiometric phases with the same crystal<br />

structures exist in different ternary subsystems with quaternary ranges of homogeneity<br />

(T­Phase in the Al­Cu­Mg system and r­ Phase in the Al­Mg­Zn system, Mg^Znn and<br />

Mg 2 Cu 5 Al6, the Laves phases in the Cu­Mg­Zn and Al­Cu­Mg systems). In modelling<br />

these phases, the model descriptions have to be compatible with regard to possible mixing<br />

in the quaternary system. Therefore, the T­phase, Laves phases and Mg2Cur,AlG in<br />

the Al­Cu­Mg system have been modelled so as to allow combination with the r­phase,<br />

­ 114 ­

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