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Effect of cooling rates on as-cast microstructures of Mg-9Al-xSi (x=1, 3) alloys
LI Xin-lin(李新林)1, 2, CHEN Yan-bin(陈彦宾)1, WANG Xiang(王 香)2, MA Guo-rui(马国睿)2
1. College of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China;
2. Centre for Biomedical Materials and Engineering, College of Materials Science and Chemical Engineering,Harbin Engineering University, Harbin 150001, China
Received 23 September 2009; accepted 30 January 2010
Abstract: The effects of cooling rates corresponding to different diameters of the steel mould and laser surface melting (LSM) on the as-cast microstructures of Mg-9Al-xSi (x=1, 3) (mass fraction, %) alloys were investigated by XRD and OM. The results show that obvious refinement of the alloy microstructure is obtained with increasing cooling rate by conventional ingot metallurgy. However, no evident modified morphologies of both dendritic primary Mg2Si and Chinese script eutectic Mg2Si in the Mg-Al-Si alloy occurs. Surprisingly, the morphologies of Mg2Si phases within the laser-melted Mg-Al-Si alloy transform drastically from both coarse Chinese script shape for the eutectic Mg2Si and dendrite for the primary Mg2Si to fine spherical particles with an average size of about 3 μm due to the rapid cooling of the melted layer, and the Mg2Si particulates distribute more uniformly in the α-Mg matrix.
Key words: Mg-Al-Si alloys; Mg2Si; modification; cooling rates; microstructure
1 Introduction
Mg-Al based alloys such as AZ91 are the most widely used magnesium alloys for structural applications, for their excellent castability and good strength. However, Mg-Al based alloys have poor creep resistance due to the thermal instability of Mg17Al12 phases[1-2]. The most common way of improving the high- temperature properties of magnesium is to induce formation of thermally stable precipitates or dispersoids as barriers to pin dislocation movement, e.g. cross slip or dislocation climb[3]. Si is an effective alloying element for such purpose since the addition of Si to Mg alloys combines with Mg to form the intermetallic compound Mg2Si which exhibits high melting temperature, low density, high hardness and low thermal expansion coefficient[4]. Thus, Mg-Al-Si based alloys have high potential as heat resistant light metals due to the excellent combination of various properties, which mainly depends on the morphology and size of Mg2Si. However, the Mg-Al-Si based alloy showed very low ductility and strength due to the formation of the coarse dendrite-shape primary Mg2Si in Mg-Si alloys with high Si content and the brittle Chinese script eutectic Mg2Si in Mg-Si alloys with low Si content during slow cooling [5-6]. It is widely known that the refinement of microstructure is mainly responsible for the improvement in the mechanical properties[7-8]. The scale of the microstructure is directly influenced by the cooling rate. Generally, rapid solidification, such as melt-spinning, spray atomization and rapid quenching [9-10], can greatly enhance the mechanical properties over conventional processing alloys of the same composition through the extension of solid solubility limits, the refinement of microstructure and the dispersion of second phase[11-12]. However, few investigations were carried out on the effect of the cooling rate on the microstructures of Mg-Al-Si alloys. The purpose of the present work is to study the as-cast microstructural evolution of the Mg-9Al-xSi (x=1, 3) alloys at different cooling rates.
2 Experimental
Mg-9Al-xSi (x=1, 3) (mass fraction, %)alloys were prepared. Commercially pure Mg, Al and Si were melted in a graphite crucible in an electric resistance furnace under the protection of a RJ-2 covering flux. The melt was stirred to assist the dissolution of the alloying elements, and then was poured into cylinder steel moulds with different diameters of 5, 10 and 25 mm after holding at 780 ?C for about 50 min. Subsequently, Mg-9Al-xSi (x=1, 3) alloys with dimensions of d25 mm× 10 mm were surface remelted by laser. The laser was employed at a scanning speed of 1.4 mm/s processing a pulse width of 25 ms, repetition frequency of 55 Hz, and pulse energy of 7 J. Ar was provided as protective gas at a pressure of 0.3 MPa. The chemical compositions of the alloy were measured with an ARL 4460 Metals Analyzer, as shown in Table 1. Metallographic samples were prepared in accordance with standard procedures, and etched with 3% HNO3 in alcohol. Microstructure and phase analyses were investigated by optical microscopy (OM) (Axiovert 200 MAT, Germany) and X-ray diffractometry (XRD) (X’Pert PRO, Holand), respectively.
Table 1 Chemical composition of Mg-9Al-xSi (x=1, 3) alloys used in this study (mass fraction, %)
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3 Results and discussion
3.1 Phase constituents
Fig.1 shows the XRD patterns of Mg-9Al-xSi (x=1, 3) alloys. There are α-Mg, β-Mg17Al12 and Mg2Si phases in both the Mg-9Al-1Si alloy and Mg-9Al-3Si alloy,
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Fig.1 XRD patterns of Mg-9Al-Si alloys: (a) Mg-9Al-1Si; (b) Mg-9Al-3Si
which agrees with the Mg-Al-Si ternary phase diagram [12].
3.2 Microstructure of Mg-Al-Si alloys
3.2.1 Effect of composition on microstructure
Figs.2(a) and (b) show the typical as-cast micro- structures of Mg-Al-Si alloys. It can be seen that the as- cast microstructures of the Mg-9Al-1Si alloys comprise α-Mg dendrites, (α-Mg+Mg2Si) eutectic with Chinese script Mg2Si embedded in the α-Mg matrix and β-Mg17Al12 precipitated discontinuously at grain boundaries; while that of the Mg-9Al-3Si alloys consist of not only the three phases mentioned above, but also Mg2Si primary dendrites that are surrounded by α-Mg sub-primary particles[13].
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Fig.2 As-cast microstructures of Mg-Al-Si alloys: (a) Mg-9Al- 1Si; (b) Mg-9Al-3Si
3.2.2 Effect of cooling rate on microstructure
Figs.3 and 4 show that microstructures of the Mg-9Al-xSi (x=1, 3) alloys at different cooling rates, different diameters of the steel mould and laser surface melting (LSM), respectively. From Figs.3(a)-(c) and Figs.4(a)-(c), there are obvious refinement of the alloy microstructure with increasing cooling rate by conventional ingot metallurgy. However, no evident modification of the morphologies of Chinese script eutectic Mg2Si in the Mg-9Al-1Si alloy occurs, while the structure of primary Mg2Si in the Mg-9Al-3Si alloy changes from equiaxial dendrites to a dendrite configuration. It should be mentioned that eutectic Mg2Si phases partially precipitate in the interdendritic region of the primary α-Mg phases due to the interdendritic
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Fig.3 Optical microscopy microstructures of Mg-9Al-1Si alloys with different diameters of steel mould ((a) 5 mm; (b) 10 mm; (c) 25 mm) and LSM treatment (d)
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Fig.4 Optical microscopy microstructures of Mg-9Al-3Si alloys with different diameters of steel mould ((a) 5 mm; (b) 10 mm; (c) 25 mm) and LSM treatment (d)
segregation caused by relatively rapid cooling. Surprisingly, it can be seen from Figs.3(d) and (d) that the morphologies of Mg2Si phases in the laser-melted Mg-Al-Si alloy transforms drastically from both coarse Chinese script eutectic Mg2Si and dendritic or equiaxial primary Mg2Si to fine spherical particles with an average size of about 3 μm due to a high degree of undercooling resulting from the rapid cooling of the laser-melted layer by LSM[14-15], which results in more uniform distribution of the Mg2Si particulates in the α-Mg matrix.
4 Conclusions
1) Obvious refinement of the microstructures of the Mg-9Al-xSi (x=1, 3) alloys was obtained by increasing the cooling rate of conventional ingot metallurgy. However, there is no obvious modification of the morphologies of dendrite-shape primary Mg2Si and Chinese script eutectic Mg2Si in the Mg-Al-Si alloy.
2) The morphologies of Mg2Si phases in the Mg-Al-Si alloy processed by LSM transforms drastically from both coarse Chinese script for the eutectic Mg2Si and dendrites for the primary Mg2Si to fine spherical particles with an average size of about 3 μm, and fine Mg2Si particulates distribute more uniformly in the α-Mg matrix in the laser melted layers.
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(Edited by FANG Jing-hua)
Foundation item: Project(LRB05-311) supported by the Postdoctoral Foundation of Heilongjiang Province, China; Project(HEUFT05038) supported by the Basic Research Foundation of Harbin Engineering University, China; Project(2009AA03Z423) supported by the National High-Tech Research and Development Program of China
Corresponding author: LI Xin-lin; Tel.:+86-451-82518173; Fax:+86-451-82518644; E-mail: lixinlin@hrbeu.edu.cn