D570
Journal of The Electrochemical Society, 154 ͑11͒ D567-D571 ͑2007͒
model for zinc deposition in acidic electrolytes.35,37 This might be
caused by the blocking effect of additives adsorbed on the electrode
surface, which led to the increase of local pH values with hydrogen
evolution. Gomes and daSalva Pereira obtained similar results.15
The quasi plateaus appeared in the polarization curves before the
rapid deposition of zinc, especially in solution SPCBT. In these po-
tential domains, the current response could be attributed to the pre-
dominant hydrogen evolution on the adsorbed species.37 Further-
more, compared with solution SPCB, the current density was much
lower in solution SPCBT, which implied that the hydrogen evolution
became slower during zinc electrodeposition in the presence of TU,
as observed by Song et al.21 This change in the lower potential
regions was mainly due to the dominant effect between TU and BA
in solution SPCBT and the partial desorption of PEG in solution
SPCB.
22 It was reported that a vigorous hydrogen evolution was able
to achieve porous copper and tin electrodeposits.39,40 Thus, as a
result of the different hydrogen evolution rate, zinc deposits pre-
pared from solutions SPCBT ͑Fig. 4͒ were evidently more compact
and homogeneous than from solution SPCB ͑Fig. 2͒.
Conclusion
Figure 6. ͑Color online͒ Polarization curves for steel electrodes in solutions
Organic compounds PEG, CTAB, BA, and TU, used separately
or in combination as additives, have great effect on the morphology
and structure of zinc electrodeposits obtained in concentrated acidic
sulfate baths by a high pulse current control.
S0, SPCB, and SPCBT
.
fore, the presence of a synergistic effect between TU and BA was
possibly due to the simultaneous formation of complexes by zinc
ions and TU and associates by TU and BA, and even involving
PEG, CTAB, and the decomposed matters of these additives.
A mixture of PEG and CTAB, compared with the separate ones,
leads to the formation of a nanocrystalline zinc coating with much
smaller grain size and burnt deposits. This mixture is able to en-
hance the solubility of BA in the concentrated zinc sulfate baths,
forming transparent baths. A mixed additive of these three com-
pounds shows a strong inhibiting effect, which promotes a shift of
zinc deposition potentials to much more negative values in compari-
son with additive-free case. As a result, bright nanocrystalline zinc
with an average grain size of 52 nm and the ͑100͒͑110͒ preferred
orientations is produced in the presence of this ternary additive.
Compared with the above ternary additive, all four compounds
used together in the plating bath can shift zinc deposition potentials
to more negative values and more powerfully inhibit the hydrogen
evolution during zinc electrodeposition. The synergetic effect of
these compounds, especially for BA and TU, is of great influence on
the zinc deposition process to achieve the grain refinement. As for
this four-additive bath, the electrodeposited zinc is bright and com-
pact, with a particle-shaped morphology, an average grain size of 43
nm, and the ͑110͒͑100͒͑201͒ preferred orientations. In addition, a
small amount of ZnO is identified in the deposits.
Polarization curves.— Bright nanocrystalline zinc coatings were
obtained from solutions SPCB and SPCBT, while only nanolaminated
zinc was produced from the base solution S0.17 Figure 6 gives the
polarization curves for steel substrates in these three solutions to
show the influence of the two mixed additives on zinc electrodepo-
sition. In addition, the polarization curves for the other six solutions
were not discussed here because the electrodeposited zinc layers had
poor appearance, especially burnt deposits.
In the case of base solution S0, a cathodic peak appeared in the
potential range −0.7 to −1.1 VSCE, which was related to the hydro-
gen evolution and formation of adsorbates ͑e.g., ZnHad, ZnOad and
ZnOHad͒.35,36 Zinc started to deposit at about −1.1 VSCE. The rapid
deposition at more negative potentials led to formation of a quasi-
vertical curve, similar to the results in Ref. 15, 37, and 38. The data
with current density larger than 50 mA cm−2 were deleted in view
of the marked ohmic drop. In solution SPCB, the analogous hydrogen
evolution peak was markedly suppressed, which could be ascribed
to the inhibitive action of organic additives, especially PEG. It was
reported that PEG could form a strongly adsorbed layer with a well-
ordered structure on the cathode surface and prevented protons from
accessing the electrode, leading to the suppression of hydrogen
evolution.22,24 However, in comparing solution SPCBT with SPCB, the
evolution peak was enhanced in the presence of TU. This was pos-
sibly due to the conflicting effect of PEG and TU in this potential
region. As mentioned above, the addition of TU to solution SP ͑i.e.,
solution SPT͒ resulted in the increase of grain size from 72 to 90 nm,
which suggested these two additives competed with each other dur-
ing the adsorption process and then gave rise to a reduction in the
overall adsorption, as observed between PEG and benzoic acid in
chloride solutions.22
Acknowledgments
Financial support provided by Natural Science Foundation of
China ͑NSFC͒ in combination with Shanghai BaoSteel Group Cor-
poration ͑grant no. 50471105͒ is greatly appreciated.
References
1. A. M. El-Sherik and U. Erb, Plat. Surf. Finish., 82, 85 ͑1995͒.
2. L. Lu, M. L. Sui, and K. Lu, Science, 287, 1463 ͑2000͒.
3. F. L. Li, B. L. Zhang, S. J. Dong, and E. K. Wang, Electrochim. Acta, 42, 2563
͑1997͒.
4. A. M. Alfantazi and U. Erb, J. Mater. Sci. Lett., 15, 1361 ͑1996͒.
5. C. Cheung, U. Erb, and G. Palumbo, Mater. Sci. Eng. A, 185, 39 ͑1994͒.
6. E. Budevski, G. Staikov, and W. J. Lorenz, Electrochim. Acta, 45, 2559 ͑2000͒.
7. U. Erb, Nanostruct. Mater., 6, 533 ͑1995͒.
8. G. Palumbo, F. Gonzalez, K. Tomantschger, U. Erb, and K. T. Aust, Plat. Surf.
Finish., 90, 36 ͑2003͒.
In solutions SPCB and SPCBT, the presence of organic mixtures
promoted a shift of the zinc deposition potential to much more nega-
tive values, i.e., about −1.56 and −1.6 VSCE, respectively. A syner-
getic effect between TU and BA created an extra overpotential of
about 40 mV. It can be inferred that the formation of bright nano-
crystalline deposits was mainly due to the high overpotentials in-
duced by the mixture additives, and the higher the overpotential the
smaller the grain size ͑Table I͒. In spite of the very high overpoten-
tial, ZnO was clearly identified, being inconsistent with the reaction
9. L. Oniciu and L. Muresan, J. Appl. Electrochem., 21, 565 ͑1991͒.
10. R. T. C. Choo, A. M. El-Sherik, J. Toguri, and U. Erb, J. Appl. Electrochem., 25,
384 ͑1995͒.
11. G. Devaraj, S. Guruviah, and S. K. Seshadri, Mater. Chem. Phys., 25, 439 ͑1990͒.
12. B. H. Juarez and C. Alonso, J. Appl. Electrochem., 36, 499 ͑2006͒.
13. Kh. M. S. Youssef, C. C. Koch, and P. S. Fedkiw, J. Electrochem. Soc., 151, C103
͑2004͒.
14. Kh. Saber, C. C. Koch, and P. S. Fedkiw, Mater. Sci. Eng. A, 341, 174 ͑2003͒.
15. A. Gomes and M. I. da Silva Pereira, Electrochim. Acta, 51, 1342 ͑2006͒.
16. Kh. M. S. Youssef, C. C. Koch, and P. S. Fedkiw, Corros. Sci., 46, 51 ͑2004͒.
17. M. C. Li, L. L. Jiang, W. Q. Zhang, Y. H. Qian, S. Z. Luo, and J. N. Shen, J. Solid
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