S.-J. Pan et al. / Electrochimica Acta 55 (2010) 2158–2162
2159
in this paper. This electrolyte was used for plain Al deposition. For
the co-deposition of Al and Zn, 1 wt% anhydrous ZnCl2 (99.99%)
was added and dissolved directly in the AlCl3–EMIC ionic liquid to
prepare a plating bath with the desired composition. All chemicals
were handled in a glove box under a purified nitrogen atmosphere.
Within the glove box, both the moisture content and the oxygen
content were maintained below 1 ppm.
1.5 V. Curve (a) in Fig. 1 displays the cyclic voltammogram obtained
in 60 m/o AlCl3–EMIC without ZnCl2 addition, in the potential range
of −0.5 to 2.5 V. As reported previously [14–16], when the AlCl3
molar ratio exceeds 50%, the following reaction takes place:
−
AlCl4− + AlCl3 → Al2Cl7
(1)
Under cathodic polarization condition, the following reaction can
occur to form metallic Al:
A diecast AZ91D Mg alloy with 9.02 wt% Al and 0.49 wt% Zn was
used as the substrate in this study. Before electrodeposition, each
sample was ground with SiC papers to a grit of 2000 inside the
glove box. A three-electrode cell controlled by an EG&G Model 273A
potentiostat/galvanostat was employed for electroplating. The Mg
alloy, with a total exposed surface area of about 0.06 cm2, was
assembled as the working electrode while an Al wire placed in a
separate fritted glass tube containing the 60 m/o ionic liquid was
used as the reference electrode. The counter electrode for plain Al
deposition was an Al spiral, which was directly immersed in the
plating bath; for Al–Zn co-deposition, a Zn spiral was used instead.
Electrodeposition was performed at room temperature under con-
stant potential mode. The potentials applied were −0.1, −0.2, −0.3,
4Al2Cl7− + 3e− → Al + 7AlCl4
(2)
−
In curve (a), there is a noticeable increase in the cathodic current
density at potentials below approximately −0.15 V, corresponding
to the reduction of the Al2Cl7− precursor in the ionic liquid to form
Al deposit. The intercept of the curves for the forward and the back-
ward scans is at approximately −0.08 V, above which Al deposition
does not occur. The existence of a cathodic current loop, as shown
for Al deposition on the glassy carbon surface. On the reverse scan,
the sharp anodic peak in curve (a) corresponds to the dissolution
of Al formed in the forward scan.
In Fig. 1, curves (b) and (c) show the cyclic voltammograms for
various potential ranges with the addition of 1 wt% ZnCl2 to the
60 m/o ionic liquid. Curve (b) depicts the cyclic voltammogram
obtained at potentials ranging from 0 to 1.5 V. The cathodic scan
shows that an abrupt increase in current density occurred at about
+0.19 V, indicating the reduction of Zn. The current loop shown in
for zinc reduction. The intercept of the reverse scan at zero cur-
rent density was found at +0.24 V, above which Zn could not be
reduced. The peak in the anodic scan is associated with the dissolu-
tion of Zn. The cyclic voltammogram for an enlarged potential scan
range of −0.5 to 2.5 V is shown as curve (c) in Fig. 1. Two cathodic
humps were observed showing the sequential reduction of Zn and
Al. The initial potential for Zn reduction, as indicated in curve (c)
was +0.19 V, identical to that revealed in curve (b). A decrease in
the current density in the first hump in curve (c) suggests that the
depletion of Zn2+ ions on the electrode surface occurred during the
cathodic scan. The potential at which the current density began
to rise again corresponds to Al reduction. As revealed in curve (a),
the reduction of Al started at potentials below −0.08 V; thus, the
co-deposition of Zn and Al can occur below this potential.
and −0.4 V, respectively, to yield a total passed charge of 50 C cm−2
.
After deposition, the samples were thoroughly cleaned with dis-
tilled ethanol and then dried in air. The surface morphologies and
chemical compositions of the deposits were examined with a scan-
ning electron microscope (SEM, Hitachi SU-1500) and its auxiliary
3. Results and discussion
Fig. 1 shows the cyclic voltammograms of a glassy carbon elec-
trode obtained at room temperature in the 60 m/o ionic liquid
with/without 1 wt% ZnCl2. The voltammograms were obtained by
scanning the potential at a rate of 0.05 V s−1 from open circuit
potential (approximately 1.0 V) towards the negative direction to
a preset value, and then reversed in the anodic direction to 2.5 or
During reverse scanning, the rates for both Al and Zn reductions
decreased. When the potential reached approximately −0.08 V,
deposition of Al ceased but Zn2+ could still be reduced until +0.24 V.
Thus, in the potential range of −0.08 to +0.24 V, the reduction of
Zn2+ to form Zn and the dissolution of Al to form Al3+ simultane-
ously took place. The (a1) peak in curve (c) corresponds to the net
current density during scanning in this potential range. The second
anodic peak (a2) is associated with the dissolution of both Al and
Zn.
formed under constant applied potential condition. The variation
of current density with time for Al deposition in 60 m/o ionic liquid
(a) in Fig. 2. The current density increased rapidly at the beginning
and then reached a steady state value at about −22.5 mA cm−2
.
With the addition of 1 wt% ZnCl2 in the 60 m/o ionic liquid, the
variation of current density with time at an applied potential of
−0.2 V is shown as curve (b) in Fig. 2. As in curve (a), a rapid
increase of the current density was followed by a steady growth
of the Al–Zn deposit. However, the steady state current density in
curve (b) is about −18 mA cm−2, lower than that of curve (a). For
a total cathodic passed charge of 50 C cm−2, the times required to
deposit Al and Al–Zn at −0.2 V were 2250 and 2640 s, respectively.
The addition of ZnCl2 decreased the deposition rate. It has been
pointed out that the ZnCl2–EMIC ionic liquids having a ZnCl2 mole
Fig. 1. Cyclic voltammograms on a glassy carbon electrode at room temperature
and at a scan rate of 50 mV S−1: (a) 60 m/o AlCl3–EMIC (scan range: −0.5 to 2.5 V),
(b) 1 wt% ZnCl2 + 60 m/o AlCl3–EMIC (scan range: 0 to 1.5 V) and (c) 1 wt% ZnCl2 + 60
m/o AlCl3–EMIC (scan range: −0.5 to 2.5 V).