102
SALAKHOVA
Table 2. Composition and quality of Re–Se coatings as functions of current density in a 1 M NaOH solution at t = 75°C
Electrolyte, mol/l
NH4ReO4 SeO2
0.05 0.05
Alloy composition, wt %
j, mA/cm2
Light gray, nonuniform
(deposition)
Re
Se
2
4
5
7
38.2
48.4
54.0
72.1
61.8
51.6
46.0
27.9
Dark gray, uniform, smooth
Black, lustrous, smooth
0.05
0.05
0.05
0.05
0.05
0.05
Dull black, smooth
External appearance of the coating
ined the temperature effect on the rate of the electrode Se. During the electrolysis of mixtures of alkaline Se and
Re solutions, the rate of ReO4– and SeO32– reduction is
process at a constant cathode potential. The results are
displayed in Fig. 4. From the slope of the lines thus
higher. This seems to be due to the depolarization effect,
obtained, we evaluated the apparent activation energy
associated mainly with the formation of the alloy. Con-
of the electrode process (Fig. 5). At potentials from
sequently, codeposition of rhenium and selenium must
−0.65 to –0.725 V, the apparent activation energy
lead to the formation of a compound or solid solution.
attains 30–35 kJ/mol. With increasing cathodic polar-
Our results demonstrate that, as the current density
rises from 2 to 8 mA/cm2, the rhenium content of the
alloy increases from 20 to 80 wt % (Fig. 7) and the
quality of the coating improves (Table 2).
At a cathode current density of 4 mA/cm2, using an
electrolyte of composition 0.05 M NH4ReO4 + 0.05 M
ization, the apparent activation energy drops to
20 kJ/mol at –0.8 V and then varies little.
Thus, at cathodic polarizations above –0.785 V,
selenium electrodeposition from alkaline electrolytes is
accompanied mainly by chemical polarization.
Since selenium deposition on the cathode is
attended by the release of a substantial amount of SeO2 + 1 M NaOH, we obtained lustrous ReSe2
hydrogen, we obtained partial polarization curves in
order to gain detailed insight into the electrode pro-
cesses involved.
Figure 6 shows the partial polarization curves for Re,
Se, and Re–Se deposition. From the curves of Re depo-
sition in elemental form and in the Re–Se alloy, it follows
that depolarization in the latter case is 350 mV (Fig. 6).
For selenium in the alloy, depolarization is 20–30 mV.
(54 wt % Re) coatings. The formation of ReSe2 was
confirmed by XRD. This compound crystallizes in the
triclinic system with lattice parameters a = 6.7275 Å,
b = 6.6065 Å, and c = 6.7196 Å. The XRD intensities
and d spacings for ReSe2 are listed in Table 3.
CONCLUSION
As seen in Fig. 1, the curves for Re–Se deposition
(curves 6, 7) lie at higher potentials than those for Re and
Codeposition of rhenium and selenium was shown
to be attended by depolarization, which is due to the
energy release upon the formation of the alloy.
Table 3. XRD data for ReSe2 obtained in an alkaline elec-
trolyte of composition 0.05 M NH4ReO4 + 0.05 M SeO2 +
NaOH (at jc = 5 mA/cm2 and t = 75°C)
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I/I0
hkl
d, Å
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INORGANIC MATERIALS Vol. 39 No. 2 2003