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COST 507 - Repositório Aberto da Universidade do Porto

COST 507 - Repositório Aberto da Universidade do Porto

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three different sections starting from binary liquid Cu-Mg alloys (50, 75, and 90 at%<br />

Mg), and one section starting from a binary liquid Mg-Y alloy (8 at% Y).<br />

The obtained experimental results for ternary liquid alloys were interpreted using an<br />

association model [82Som2, 90Som]. It was found that a good description was possible<br />

with the assumption of three binary associates (Cu 2 Mg, CuY, Mg 2 Y). With the model<br />

parameters obtained from the three limiting binary systems it was possible to calculate<br />

thermodynamic properties for ternary liquid alloys. Although there are some<br />

indications for ternary interactions, the existing experimental <strong>da</strong>ta are still not<br />

extensive enough to warrant a corresponding evaluation. All experimental details and<br />

the final results are summarized in Appendix 2 and are published as [97Gan2].<br />

4 The Ternary Cu-Mg-Si System<br />

4.1 Thermodynamic Properties<br />

Magnesium vapor pressures were determined along an isopleth with a constant concentration<br />

ratio of Xcu/xsi = 7/3 using again the described isopiestic method [93Gna]. This<br />

particular composition was selected because of a minimum melting temperature of<br />

802°C at the eutectic point (30 at% Si) in the Cu-Si binary system [8601e]. It was<br />

supposed to guarantee a maximum stability range of the liquid phase in the corresponding<br />

ternary section which, however, was reduced considerably by the appearance<br />

of a melting point maximum of about 950°C around 33 at% Mg and 13 at% Si [39Wit,<br />

60Asc]. From the vapor pressure measurements, partial thermodynamic properties of<br />

magnesium were derived; they are presented for a temperature of 1173 K. A Gibbs-<br />

Duhem integration was performed based on the method of Peiton and Flengas [69Pel],<br />

using the obtained magnesium activities to calculate integral Gibbs energies of mixing<br />

for liquid alloys in the investigated isopleth.<br />

The enthalpy of mixing in this isopleth with Xc u /x s ¡ = 7/3 was determined by solution<br />

calorimetry [80Som]. Measurements were performed starting both from liquid binary<br />

Cu 0 7 Si 0 3 -alloys (and adding solid magnesium) and from liquid magnesium (adding<br />

solid Cu 07 Si 03 -samples). Partial enthalpies of mixing of magnesium were derived from<br />

the obtained <strong>da</strong>ta and were found to be in very good agreement with those derived<br />

from the temperature dependence of the magnesium activities.<br />

The obtained thermodynamic results are again interpreted by the described association<br />

model [82Som2, 90Som]. All experimental details as well as the final results can be<br />

found in Appendix 3 and will be published soon [97Gan3].<br />

4.2 Phase Diagram<br />

The Cu-Mg-Si phase diagram along the isopleth with XcAsi = 7/3 was studied by<br />

means of differential thermal analyses (DTA) and X-ray powder diffraction methods.<br />

With these it was possible to derive the shape of the liquidus curve. The phase<br />

relationships at lower temperatures are very complicated (see also [60Asc]), and it was<br />

found that additional measurements will be necessary outside the investigated section<br />

- 60 -

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