COST 507 - Repositório Aberto da Universidade do Porto
COST 507 - Repositório Aberto da Universidade do Porto
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 />
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