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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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 />
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