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COST 507 - Repositório Aberto da Universidade do Porto

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deviation from Kopp­Neumann' s rule derived by [92Aga] from the temperature dependence<br />

of the enthalpy of mixing of the liquid, but the numerical value is refined to about<br />

70% of that assessed by [92Aga].<br />

Kowalski and Spencer [93Kow] in the Cu­Zn system assumed different lattice stabilities<br />

for pure Zn in its stable state (hep with c/a = 1.856) and as hep phase with axial ratio<br />

c/a = 1.556 (c­Cu­Zn phase), which lies close to the ideal axial ratio c/a = 1.633. To<br />

get compatibility, in Mg­Zn the Mg(hcp) solid solution had to be reformulated to show<br />

the same lattice stability for the end member pure Zn as [93Kow] used for the t­Cu­Zn<br />

phase.<br />

Furthermore the MgZn2 Laves phase should be modelled similarly as MgCu 2 with antistructure<br />

atom formation on both sublattices, although the only information for that is<br />

the vague statement: "The homogeneity range of MgZn 2 is about 1 at.%" [90Mas].<br />

The Mg­Zn system was re­optimized using the experimental­<strong>da</strong>ta file of [92Aga] and<br />

the new C p^u' d and<br />

<strong>da</strong>ta of [95Som] (Fig.2). The Laves phase parameters °¿Mgfzn,M g<br />

^Mg.ziîrZn were estimated by trial and error to reproduce a maximum homogeneity range<br />

of 1 at.% for MgZn 2 .<br />

2.4 The Mg­Si System<br />

The enthalpy of formation and melting as well as heat capacity of Mg2Si were measured<br />

calorimetrically by [97Feu]. The Mg­Si system was re­optimized using the experimental<strong>da</strong>ta<br />

file of [92Cha] together with the new <strong>da</strong>ta of Mg 2 Si [97Feu].<br />

2.5 The Al­Mg­Si System<br />

New measurements on this system were carried out by F. Sommer's group at MPI<br />

Stuttgart. The Al corner of the Al­Mg­Si ternary system was investigated by DTA<br />

and optical micrography. A few points of the solvus of the (Al) solid solution were<br />

precisely determined by dilatometry. The results of these experiments and the up<strong>da</strong>ted<br />

Mg­Si system together with literature <strong>da</strong>ta were used to redetermine a complete set of<br />

analytical descriptions of the Gibbs energies of all stable phases of the Al­Mg­Si system.<br />

The technically most important part, the solvus surface of the (Al) solid solution<br />

could be improved (Fig. 3). A publication of this re­optimization is in press [97Feu] .<br />

2.6 The Cu-Mg-Zn System<br />

The assessment of the Cu­Mg­Zn system is mainly based on the critical review of experimental<br />

literature provided by <strong>COST</strong> <strong>507</strong>, Coordination group B [94Gho]. The Cu­<br />

Mg­Zn phase diagram is characterised by the formation of three Laves phases MgCu2,<br />

MgZn 2 and the MgNi 2 ­type phase Mg 2 CuZn,3 (τ), which have large solubility ranges.<br />

­ 116 ­

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