The previous update on this ternary system by [2007Rag] reviewed mainly the thermodynamic assessment of [1998Lia]. Very recently, [2009Ren] determined a partial isothermal section at 360°C for Cu-lean alloys and found that Cu stabilizes the miscibility gap of the Al-Zn fcc phase.
Binary SystemsThe Al-Cu phase diagram [2004Ria] depicts the following intermediate phases: CuAl 2 (C16-type tetragonal, denoted h), CuAl(HT) (g 1 , orthorhombic) CuAl(LT) (g 2 , monoclinic), Cu 5 Al 4 (HT) (f 1 , orthorhombic, space group Fmm2), Cu 5 Al 4 (LT) (f 2 , orthorhombic, space group Imm2), e 1 (HT) (cubic?), e 2 (LT) (B8 1 , NiAs-type hexagonal), Cu 3 Al 2 (rhombohedral), Cu 9 Al 4 (HT) (c 0 , D8 2 , Cu 5 Zn 8 -type cubic), Cu 9 Al 4 (LT) (c 1 , D8 3 , Cu 9 Al 4 -type cubic), and Cu 3 Al (b, bcc). The Al-Zn phase diagram [1993Che] contains no intermediate phases. A miscibility gap occurs in the Al-based face centered cubic (fcc) solid solution below 351°C, where the fcc phase splits into fcc 1 and fcc 2 . The monotectoid reaction fcc 2 M fcc 1 + (Zn) follows at 277°C. The Cu-Zn phase diagram [1993Kow, Massalski2] is characterized by a series of peritectic reactions, which yield CuZn (b, bcc), Cu 5 Zn 8 (c, D8 2 -type cubic), CuZn 3 (d, B2, CsCl-type cubic), and CuZn 4 (e, cph). Zn (cph) has a c/a axial ratio much larger than e and the two coexisting cph phases are modeled separately with different interaction parameters [1993Kow]. The b phase orders to a CsCl-type B2 phase (b¢) through a second-order transition below $460°C.
Ternary PhasesA ternary phase with rhombohedral symmetry and with the nominal composition Al 4 Cu 3 Zn (denoted s) is known in this system [Pearson3]. The homogeneity range of s and its temperature dependence are not clearly defined. The structurally-related, low-temperature form s¢ was found to be stable by [2005Hao] between 400°C and room temperature.
Ternary Phase EquilibriaWith starting metals of 99.999% purity, [2009Ren] prepared diffusion couples of Cu-Zn master alloys with pure Al. The diffusion couples were annealed at 360°C for 48 h and quenched in water. The coexisting phase compositions were measured by electron probe microanalysis and listed. The isothermal section at 360°C constructed by [2009Ren] is shown in Fig. 1. In the Al-Zn system, the miscibility gap in the fcc phase closes at 351°C. The addition of Cu stabilizes this gap, which is stable at 360°C, even with as low as 0.1 at.% addition of Cu. The gap increases in width with increasing Cu content. In an earlier study, [2004Ren] determined tie-lines between fcc 1 and fcc 2 at 340 and 320°C for small additions of Cu and these are shown in Fig. 2. The Cu addition shifts the fcc 1 /(fcc 1 + fcc 2 ) and (fcc 1 + fcc 2 )/fcc 2 phase boundaries towards the Al-rich corner. Also, Cu segregates in the fcc 2 phase in preference to fcc 1 .The computed results of [2009Dai] indicate that the stabilizing effect of Cu on the Al-Zn miscibility gap increases with increasing Cu content, culminating in a metastable miscibility gap in the Al-Cu binary system...