# Electrochemical Behavior of Zn-Ni Alloys in Borate Buffer Solutions

Authors: Ayman M. Zaky; Fawzi H. Assaf; Fatma El Zhraa A. H. Ali
Journal: ISRN Materials Science
 (2011)

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## Abstract

The Electrochemical behavior of Zn-Ni alloys was studied in borate solutions using cyclic voltammetry, potentiodynamic anodic polarization, and current transient techniques under the effect of alloy composition, stepwise increasing potential, scan rate, and electrolyte concentration. The voltammogram consists of two potential regions separated by the critical potentialEcrit. The first potential region involves the selective dissolution of the less noble metal, zinc, and the appearance of two anodic peaks A1 and A2. Peak  A1 is due to  the formation of Zn(OH)2 and A2 to the formation of ZnO on the alloy surface. The second potential region relates to the simultaneous dissolution of nickel. This region was characterized by the appearance of three anodic peaks A3, A4, and A5 prior to the oxygen evolution reaction. These peaks are assigned to the formation of Ni(OH)2, NiOOH, and Ni2O3, respectively. The anodic voltammetric profiles of the alloys lies below those of the pure metals indicating decreased rates of dissolution of the two metals, zinc and nickel, from the alloys. On alloying with nickel, the rate of zinc dissolution was decreased which increases its protective life as sacrificial anode for automobile body against corrosion. X-ray diffraction analysis confirmed the existence of Zn(OH)2, ZnO, Ni(OH)2, and Ni2O3 with preferred orientations (008), (101), (002), and (202) of the alloy surface polarized to noble potentials. Potentiostatic current/time transients showed that the formation of Zn(OH)2, ZnO, Ni(OH)2, NiOOH, and Ni2O3 layers involves a nucleation and growth mechanism under diffusion control.


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## Body

## 1. Introduction

The anodic behavior of zinc in Na2B4O7 solutions has been investigated by the galvanostatic polarization technique. The polarization curves are characterized by one distinct arrest corresponding to Zn(OH)2 or ZnO, after which the potential increases linearly with time before reaching the oxygen evolution region [1]. It is generally accepted that Zn passivation begins with the precipitation of the zincate ion as Zn(OH)2 or ZnO [2–5]. Powers and Breiter [6] examined the surface of Zn optically during potentiodynamic oxidation in stationary KOH solution. They noted the existence of two different precipitates [2] suggested that the first one was Zn(OH)2 and the second ZnO. The electrochemical behavior of zinc in NaOH solutions was investigated [7] by using potentiodynamic technique and complemented by X-ray analysis. They found that E/i curves exhibit active, passive, and transpassive regions prior to reaching the oxygen evolution potential. The active region displays two anodic peaks. The passivity is due to the formation of a compact Zn(OH)2 film on the anode surface. The transpassive region is assigned to the electroformation of ZnO.In spite of the earlier studies, there remains considerable disagreement in the literature on the interpretation of the nature and the mechanism of the anodic layers on nickel [8, 9] considered the presence of Ni(OH)2 in the film. The anodic oxidation of nickel electrode in alkaline solutions in the potential ranges related to the Ni/Ni(OH)2, and Ni/NiOOH redox reactions have been studied under galvanostatic and potentiodynamic conditions. However, there is a general agreement that when nickel is immersed in alkaline solutions, spontaneous dissolution of the metal occurs followed by the formation of Ni(OH)2 [10] film.    Recently [11] confirmed that the film formed in the passive region is composed of NiO (inner) and  Ni(OH)2 (outer) in borate solutions, NiO being the passivating species. At potentials above a critical value, the β-Ni(OH)2 film is converted  to an Ni(III) oxide phase, identified by ellipsometry as β-NiOOH [12]. The conversion of β-Ni(OH)2 to β-NiOOH is a complex process.The aim of this study was to investigate the effect of alloying zinc with nickel on increasing the life time of sacrificial anodic protection of zinc for automobile body against corrosion. The electrochemical behavior of Zn-Ni alloy in  0.15 N of borate solution. The voltammetric profiles of pure Zn and pure nickel were included for comparison. The microstructure and composition of the passive film formed during the anodic sweep were characterized by X-ray diffraction analysis.


## 2. Experimental

Three zinc-nickel alloys (Table1), pure zinc and pure nickel (99.99% pure supplied by Merck), were used in studying the cyclic voltammetric behavior of zinc-nickel alloys in 0.15 N of borate buffer solution. The alloys were made in the Aluminum Company of Egypt by fusing appropriate amounts of the two components in a graphite crucible at a desired temperature. They were cooled and made into cylindrical rods with a cross-sectional area 0.126 cm².Table 1
Composition of the studied alloys.
AlloyZn%Ni%I95.05.0II90.010.0III85.015.0All of the electrodes were mounted in Teflon so that only the cross-sectional area of 0.126 cm² was in contact with solution. Before each experiment, the working electrode was polished with successively finer grades of emery paper and then with alumina paste to obtain a mirror-like surface finish then degreased with ethyl alcohol and rinsed with doubly distilled water. Then, the electrodes were transferred to the solution where they were left at −2000 mV for 1 min, to remove any oxide present, before running the experiments.The solutions used were prepared from Analar grade chemicals. All experiments were performed using freshly prepared solutions and freshly polished electrodes. The electrolytic cell used was of 100 cm³ capacity and consisted of three separate compartments, which were used for the working, counter, and reference electrodes. the counter electrode was a rod of graphite while the reference electrode was a saturated calomel electrode (SCE). The cyclic voltammetric polarization was applied by means of EG&G potentiostat/Galvanostat Model 273A using the 352 SoftCorr III software on a Pentium II computer. The morphology of the alloy surface in the potential range beyond the critical potentialEcrit was monitored by SEM using a Philips model XL-200 instrument operated at 15 keV. The composition of the corrosion products formed on the alloy during anodic polarization was investigated by XRD analysis using a Philips P. W. Model 1730.


## 3. Results and Discussion

The electrochemical behavior of Zn-Ni alloys was studied in 0.15 N boric acid and 0.15 N borax (borate buffer solution) using cyclic voltammetric technique, and the data are given in Figure1. The voltammograms were recorded between the starting cathodic potential Ec = −1600 mV and switching potential Ea = 1300 mV at scan rate of 50 mVs−1. The cyclic voltammetric behavior of pure zinc and pure nickel were introduced for comparison. In Figure 1, curve 1 represents the voltammetric behavior of pure Zinc. The anodic excursion exhibits two anodic peaks A1 and A2 in the active region before the onset of passivation. The two anodic peaks are related to the formation of the anodic peak A1 that is related to the formation of Zn(OH)2 while the anodic peak A2 is related to the formation of ZnO [2], (1)Zn+2OH-⟶Zn(OH)2+2e-(2)Zn+2OH-⟶ZnO+H2O+2e-.Figure 1
Cyclic voltammograms of (1) Zinc, (2) Nickel, (3) alloy I, (4) alloy II, and (5) alloy III in 0.15 N of borate buffer solution at 25°C and 50 mVs−1.Curve 2 represents the cyclic voltammetric behavior of pure nickel in 0.15 N of borate buffer solution. The forward sweep is characterized by the appearance of three anodic peaksA3, A4, and A5 which are ascribed to the formation of Ni(OH)2, NiOOH [13], and Ni2O3 [14], respectively,  as shown in (7) and (8), respectively, (3)Ni+2OH-⟶Ni(OH)2+2e-(4)Ni(OH)2+OH-⟶NiOOH+H2O+e-.Visscher and Barendrecht [15] examined the growth of oxide layer on Ni surface in alkaline solutions using cyclic voltammetry. They found that the first anodic film is a thin layer of NiO·nH2O which transfer to Ni(OH)2 on increasing the anodic potential, on the other hand De Souza et al. [16] suggested that the first layer of  NiO is covered after the anodic scan to a thick film of β-Ni(OH)2. At potential above a critical value, the β-Ni(OH)2 film is converted to β-NiOOH [5]. However, on reversal polarization, β-NiOOH is reduced back to β-Ni(OH)2. The reduction of NiOOH to Ni(OH)2 was observed also in carbonate ions [17]. The backward sweep was characterized with the appearance of two cathodic peaks C2  and C3 which are ascribed to the reduction of NiOOH to Ni(OH)2 and Ni2O3 to Ni(OH)2.The cyclic voltammetric behavior of alloys I, II, and III is represented in Figure1 curves 3, 4, and 5, respectively. On sweeping the potential in the positive direction, the forward sweep is characterized by the appearance of two potential regions separated by the critical potential Ecrit: (i) the selective dissolution potential and (ii) the simultaneous dissolution potential region. It seems that the alloys anodic profiles in these regions lay below those of two pure metals as an indication of decreasing the rates of metals dissolution from these alloys with increasing the nickel content. In the subcritical potential region, selective dissolution of the less noble component, zinc, occurs and results in the appearance of the two anodic peaks A1 and A2. Visual inspection shows that these anodic peaks are related to the formation of Zn(OH)2 and ZnO, respectively. Considering the content of zinc in the alloys, it seems that the processes involved in the appearance of the anodic peaks A1 and A2, that is, selective dissolution of zinc and formation of  Zn(OH)2 and ZnO, are decreased as shown by decreasing the heights of the anodic peaks A1 and A2 with increasing nickel content in the alloy. The peak potentials of the anodic peaks A1 and A2 were shifted towards more active, negative values with increasing nickel content in the alloy as an indication of enhancing the dissolution of zinc from the alloy; see, (1) and (2), (5)ZnxNiy+2OH-⟶Znx-1Niy+Zn(OH)2+2e-(6)Znx-1Niy+2OH-+⟶Znx-2Niy+ZnO+H2O+2e-.The potential region II was characterized by the appearance of three anodic peaksA3, A4, and A5. Visual inspection shows that the anodic peaks A3 and A4 are related to the formation of Ni(OH)2 and NiOOH [13] and Ni2O3 [14], respectively,(7)Znx-2Niy+2OH-⟶Znx-2Niy-1+Ni(OH)2+2e-(8)Ni(OH)2+OH-⟶NiOOH+H2O+e-.X-ray diffraction analyses of Zn-Ni alloys at potential values noble to the potential region of the anodic peakA2 and at potential more noble that of peak A4 are shown in Figures 2 and 3 for alloys II and III, respectively. Figure 2 shows the existence of ZnO and Zn(OH)2 with preferred orientations (101) and (224), respectively, on the surface of alloy II. Also, Figure 3 shows the presence of Zn(OH)2, ZnO, Ni(OH)2, and Ni2O3 with preferred orientations (008), (101), (002), and  (202), respectively, on the surface of alloy III. From these results, it appears that the initial stage of the anodic oxidation of Zn-Ni alloys involves selective dissolution of less noble metal component (zinc). It seems that NiOOH is dehydrated later during the movement of the electrode to carry out XRD analysis to Ni2O3,(9)2NiOOH⟶Ni2O3+H2OFigure 2
X-ray diffraction pattern of  alloy I surface potentiodynamically polarized to −600 mV at 25°C and 50 mVs−1.Figure 3
X-ray diffraction pattern of alloy III surface potentiodynamically polarized to 1300 mV with at 25°C and 50 mVs−1.The complementary relationship between the anodic and the cathodic peaks was obtained by reversing the potential at different step potentialsEs (Figure 4). When Es lies between the potential of the anodic peaks A1 and A2, only the cathodic peak C1 appears which is ascribed to the reduction Zn+2 species to Zn. No more cathodic peaks appear on reversing the potential at values noble to the anodic peak A2. On reversing the potential at nobler values, the peak current density of the cathodic peak C1 was increased, and its peak potential was displaced towards more negative values.Figure 4
Cyclic voltammograms of alloy I in 0.15 N of borate buffer solution at 25°C, scan rate 50 mVs−1, and various reversing anodic potentials: (1) −900 mV, (2) −300 mV, (3) 350 mV, (4) 900 mV, and (5) 1300 mV.The effect of increasing sweep rate was studied for the three alloys in 0.15 N of borate buffer solution at 25°C. Figure5 represents the cyclic voltammetric behavior of alloy I at different sweep rates. It seems that increasing sweep rate increased the peak potential  of all anodic peaks and shifted their potentials in the positive direction. Figure 6 represents the linear dependence of the peak current density of the anodic peaks on the square root of the sweep rate for the alloy I where straight lines passing by the origin are obtained. The linear relations indicate that the processes involved the appearance of these peaks are diffusion-control processes. For a diffusion-controlled process, the peak current ip(Ax) is related to the scan rate by the following equation [18]:(10)ip=abz1/2cD1/2ν1/2,Figure 5
Cyclic voltammograms of alloy I in 0.15 N of borate buffer solution at 25°C and various scan rates; (1) 25 mVs−1, (2) 50 mVs−1, (3) 100 mVs−1, (4) 125 mVs−1, and (5) 150 mVs−1.Figure 6
Relation between the peak current density,ip, and the root of scan rate for the anodic  peaks for alloy I in Borate buffer solution: (1) A1, (2) A2, (3) A3, and (4) A4.wherea and b are constant, C is concentration of the diffusive species, D is the diffusive coefficient of the diffusing species, and z is the number of the exchanged electrons.The cyclic voltammetric behavior of Zn-Ni alloys at 25°C and at scan rate 50 mVs−1 was examined in different concentration of borate buffer solution, and the results of alloy I is given in Figure 7. The peak current densities of the anodic peaks were increased, and their corresponding potentials are shifted towards more negative values with increasing the borate buffer solution concentration. Figure 8 represents the linear relationship between logCNa2B4O7 and logip of the anodic peaks of the alloy I.Figure 7
Cyclic voltammograms of alloy I at 25°C scan rate 50 mVs−1 and in various concentrations of  borate buffer solutions; (1) 0.1 N, (2) 0.15 N, (3) 0.2 N (4) 0.25 N and (5) 0.4 N.Figure 8
Relation between the peak current density of the anodic peaks,ip, and logC[H3BO3+Na2B4O7] for alloy I; (1) A1, (2) A2, (3) A3 and (4) A4.In order to get more information about the electrochemical behavior of Zn-Ni alloys in borate buffer solution, potentiostatic current/time were performed at different anodic stepsEs. Figure 9 shows the current transients for alloy I in 0.15 N of borate buffer solution at 25°C. It seems that the current time transient densities decrease monotonically with time to reach a steady state value. The more positive potential, the steady current, increases as an indication of increasing in the thickness of anodically formed layer. The continuously decreasing parts of the current transients fit linear i versus t-1/2 relationships, Figure 10, going through the origin and showing interesting features. When Es=-900 mV, the plot consists of two portions with each one obeyed a linear relationship, which represent the formation of two layers. These layers are Zn(OH)2, ZnO. When Es=-600 mV, the plot consists of three portions with each one obeyed a linear relationship, which represent the formation of two layers. These layers are Zn(OH)2, ZnO, and Ni(OH)2. If Es at 200 mV, the data represent a plot consisting of four portions as a result of the formation of four layers, which are Zn(OH)2, ZnO, Ni(OH)2, and NiOOH. Similarly, if Es is held at 1000 mV, the data represent plots consisting of five portions as an indication of the four layers. The fifth layer is probably Ni2O3. The formation of these five layers involves a nucleation and growth mechanism under diffusion control.Figure 9
Current transients versus time recorded for alloy I in 0.15 N of Borate buffer solution at 25°C and constant anodic step potentials; (1) −900 mV, (2) −600 mV, (3) 200 mV and (4) 1000 mV.Figure 10
Dependence of the current density ont-1/2 for the descending portions of the current transients for alloy I in 0.15 N of Borate buffer solution at 25°C: (1) −900 mV, (2) −600 mV, (3) 200 mV, and (4) 1000 mV.


## 4. Conclusions

(1)
The cyclic voltammetric behavior of zinc-nickel alloys was studied in 0.15 N of borate buffer solution  using cyclic voltammetry, anodic polarization, and current time/transient techniques.(2)
The anodic voltammetric profiles of the alloys lie below those of the pure metals indicating decreased rates of dissolution of the two metals, zinc and nickel, from the alloys. On alloying with nickel, the rate of zinc dissolution was decreased which increases its protective life as sacrificial anode for protecting automobile body against corrosion.(3)
The forward sweep was characterized by the appearance of five anodic peaks corresponding to the formation of Zn(OH)2, ZnO, Ni(OH)2, NiOOH, and Ni2O3 before oxygen evolution takes place.(4)
The backward sweep shows two cathodic peaks in pure nickel corresponding to the reduction of Ni2O3 and NiOOH to Ni(OH)2, the backward sweep in alloys shows only one cathodic peak due to the reduction of  Zn+2 species to Zn.(5)
A study of the effect of scan rate has shown that the dissolution processes in the regions of the anodic peaks in the alloys are under diffusion control.(6)
Potentiostatic current/time transient measurements reveal that the formation of Zn(OH)2, ZnO, Ni(OH)2, NiOOH, and Ni2O3 layers involves a nucleation and growth mechanism under diffusion control.



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*Source: 356863-2011-08-03.xml*