EIS and potentiodynamic polarization studies on immiscible monotectic Al–In alloys
Introduction
A number of Al-based monotectic binary alloys having limited solubility in the liquid state have significant potential for many industrial applications, such as electronic components, high temperature superconductors, self-lubricated bearings [1], [2], [3], [4], [5] and optical devices [6]. Serious problems can be associated with conventional melting and casting techniques of these alloys, caused by severe gravity segregation in casting due the large densities differences between the liquid phases [2], [5]. It is important to remark that Al-based monotectic alloys have an Al-rich liquid phase L1, at the monotectic temperature, which is decomposed into an Al-rich solid phase S1 and a liquid phase L2. During cooling, a continuous Al-rich matrix is formed with the liquid minority phase being retained in a discontinuous way within the solid matrix in the form of isolated pockets [5], [7]. The competition between the growth of the minority phase and the rate of displacement of the solidification front will determine if the prevalent morphology of the microstructure will be characterized by fibers or droplets [7].
Kamio et al. [8] reported the development of the microstructure of a monotectic Al–17.5 wt.% In alloy during the steady-state growth in an unidirectional solidification set-up at various growth rates and temperature gradients. The resulting microstructures were shown to be formed either by small indium droplets or by fine and regularly aligned fibers along the growth direction disseminated in the Al matrix, which depended on the range of thermal gradients and growth rates imposed during solidification. They reported that the droplet morphology prevailed when a growth rate of about 1.1 × 10−6 m/s was attained. Kamio et al. [8] have also compared their experimental results of interphase spacing and growth rate with those reported in studies by Grugel and Hellawell [9], [10]. It was shown that the interphase spacing decreases with the increase in the growth rate [8], [9], [10]. Yasuda et al. [4] used a static magnetic field in order to control the monotectic solidification of Al–In alloys. They observed the presence of both indium rods and droplets segregated close to the bottom of the casting [4]. Liu et al. [2] have shown that the size of indium particles increased with the increase in distance from the chilled surface.
Despite the potential for the use of Al–In alloys in a number of industrial applications, the literature is scarce on studies interrelating microstructural effects such as the morphology of the indium particles and the interphase spacing to the corresponding electrochemical corrosion behavior. It is expected that the control of the resulting microstructural array of a monotectic Al–In alloy would permit to prescribe guidelines with a view to preprogramming a required corrosion resistance.
The present study focus on the effect of the scale of the interphase spacing of a microstructure, formed by indium droplet-like particles embedded in an Al-matrix, on the resulting EIS and potentiodynamic polarization plots of a monotectic Al–In alloy, with tests performed into a naturally stagnant 0.5 M NaCl solution at 23 (±3) °C.
Section snippets
Specimens preparation
Al–5.5 wt.% In alloy samples were prepared using commercially pure (c.p.) Al (99.8 ± 0.13 wt.%) and In (99.9 ± 0.01 wt.%). The main impurities were determined by Energy Dispersive X-ray Spectroscopy (EDS) coupled with SEM, and confirmed through an X-ray fluorescence technique. The results, shown in Table 1, are average values, which are based on measurements carried out in different samples.
In order to obtain directionally solidified Al–5.5 wt.% In alloy samples, a water-cooled transient solidification
Microstructure array
Fig. 2(a)–(e) shows typical microstructures of Al–In alloy samples from five different positions in the casting (10, 15, 50, 60 and 70 mm from the cooled bottom). It can be seen that from the casting surface (cooled bottom) up to a position (P) of about 40 mm, the microstructure is characterized by a mixture of cells and indium droplets and for P > 40 mm only In-droplets prevail. The cellular (λc), and interphase spacings (λ) were measured according to the schematic representation shown in Fig. 3(c).
Conclusions
The following conclusions can be drawn from the present experimental investigation:
- 1.
The experimental results have shown that for regions closer to the casting surface (higher cooling rate, about 5 °C/s), the droplet-like indium particles have the lowest diameters (i.e. between 600 nm and 900 nm coexisting with a average cell spacing (λc) of about 20 (±8) μm). The size of these droplets is associated with the driving-force determining the corrosion resistance (current density). This is attributed to
Acknowledgements
The authors acknowledge the financial support provided by FAEPEX-UNICAMP, CNPq (The Brazilian Research Council) and FAPESP (The Scientific Research Foundation of the State of São Paulo, Brazil).
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