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COST 507 - Repositório Aberto da Universidade do Porto

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appearance of this phase at 13.5 wt% Si. Our measurements indicate that this phase is<br />

not precipitated in equilibrium at Si contents below 20wt%, however the phase may be<br />

readily nucleated at lower Si contents under non equilibrium solidification conditions<br />

[93Sim].<br />

2.3 Growth of Large Crystal<br />

In order to establish the enthalpy of the two important ternary phases, alpha and beta,<br />

in the Al-Mn-Si system, a program was initiated at SINTEF to grow large crystals of<br />

these phases. Since these are peritectic phases, they could not be made simply by<br />

mixing appropriate amounts of Al, Mn and Si and having them react at high<br />

temperature in the liquid state. On the other hand the reaction kinetics in the solid state<br />

forms a serious barrier to achieving single phase samples with a homogenous<br />

composition on a practical time scale, at lower temperatures. The only possible<br />

approach was therefore to grow the alpha and beta crystals in the two phase liquid +<br />

alpha (or beta) region. Subsequently the samples were quenched to room temperature<br />

to minimise the problem of nucleation of other phases on the existing crystals during<br />

solidification. After dissolution of the aluminium matrix we were left with millimetre<br />

sized crystals of the desired phases [96Sim]. Attempts to measure the heat of formation<br />

of these phases are underway at the Université Paris Sud.<br />

A spin-off result of this investigation has been to question the results reported by Pratt<br />

and Raynor [51Pra]. In the round I assessment of the Al-Mn-Si system, heavy<br />

emphasis was placed on the results of Pratt and Raynor, with regard to the stability of<br />

the beta-AlMnSi phase. The present experimental investigation has, however, not<br />

succeeded in reproducing this earlier work. An attempt to grow the beta phase<br />

according to the same procedure as was employed by Pratt and Raynor [51 Pra] was<br />

unsuccessful. Unfortunately this experiment resulted in a beta core surrounded by an<br />

alpha shell, indicating that the beta phase was the primary phase but that the holding<br />

temperature was in the liquid + alpha phase region [96Sim]. This observation has lead<br />

to some <strong>do</strong>ubt as to the reliability of [51 Pra], which is currently being incorporated in<br />

the reassessment of Al-Mn-Si [97Ran].<br />

3 Calculations<br />

Even though most of the work involved was completed in round I of the <strong>COST</strong><strong>507</strong><br />

action the completion of our evaluation of the Al-Fe-Si [93Sei] and Al-Mn-Si [93Kol]<br />

systems took place during round II. The Al-Mn-Si system has been subject to extensive<br />

experimental and computational réévaluation during the course of round II as reported<br />

by Rand et al [97Ran]. No detail will therefore be given in this report.<br />

In the case of the Al-Fe-Si system, the assessment by Seiersten [93Sei] remains as the<br />

accepted <strong>COST</strong><strong>507</strong> evaluation. The work is therefore detailed here.<br />

3.1 The Al-Fe-Si Assessment<br />

The central part of the assessment is based on experiments by Take<strong>da</strong> and Mutuzaki<br />

[40Tak]. This is the only complete determination of the phase diagram, and later<br />

164

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