Abstract
Electroplated Ni–Co alloys show superior electrocatalytic activity towards hydrogen evolution reaction. In this work, the cysteine and sodium gluconate obtained from natural products were utilized to electroplate the nanocrystalline Ni–Co alloys. The electroplating baths were characterized using cathodic polarization technique. The effect of sodium gluconate, cysteine and boric acid on the surface morphology of the electroplated Ni–Co alloys was studied using scanning electron microscopy (SEM). Chemical composition of the electroplated Ni–Co alloys was determined using the energy dispersive X-ray (EDX), and their crystal lattice system was examined by X-ray diffraction (XRD) analysis. The X-ray diffraction pattern confirms that the electroplated Ni–Co alloys with Co% of 1–75% arranged in face-centred cubic (FCC) structure, while the electroplated Ni–Co alloys with Co% more 76% positioned in hexagonal closed-package (HCP) structure. The thickness of the Ni–Co alloys varied between 14.61 and 27.94 µm. The cathodic polarization data show that gluconate and cysteine enhance electroplating of Ni–Co alloys by decreasing the overpotential of Ni2+ and Co2+ reduction reaction. Potentiodynamic polarization was utilized to study the electrochemical behaviour of the Ni–Co alloys in NaOH aqueous solutions, which indicated that electroplated Ni–Co alloys with low Co% displayed the low rate of corrosion.
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1 Introduction
Electroplating of metals and alloys has great interests for various applications. Electroplated Ni alloys possess high electrocatalytic activity, superior mechanical properties, corrosion resistance, thermo-physical and magnetic properties [1,2,3]. Nanocrystalline Ni alloys have been used as cathodes for the hydrogen evolution reaction [4,5,6,7,8]. In addition, Ni alloys are characterized by the high hardness and the superior corrosion resistance, which is likely to be substituted for hard alloys such as hard chromium materials [9]. Moreover, nickel alloys have good resistance to corrosion under atmospheric, aqueous neutral pH and deaerated non-oxidizing acidic medium. In addition, Ni–Co alloys show superior resistance to corrosion in caustic alkalis [10, 11] and can be utilized as cathodes for hydrogen evolution reaction.
Electroplated Ni alloys can be greatly influenced by different chemical additives which can produce a dense thin film for corrosion protection of different substrates in alkaline solution. The effect of different additives such as gluconate, boric acid, and cysteine on the electroplating of Ni–Co alloys is investigated during this study. Additives such as complexing agent, brighteners and antipitter can improve to a great extent the mechanical and surface morphology of the electroplated Ni–Co alloys. Electroplating of Ni–Co alloys was performed using the organic refiner such as saccharin which led to the formation of nanocrystalline structures [12]. Most hard Ni coatings produced using the electroplating technique had high tensile intrinsic stress [13]. Addition of straight-chain organic sulphur compounds decreases the stress and produces dense and smooth coatings. The natural mercapto compounds such as cysteine produce bright and fine granular coatings. The present work studies the electroplating of Ni–Co alloys using gluconate-cysteine bath under the galvanostatic condition and investigates the electrochemical behaviour of the electroplated Ni–Co alloys in sodium hydroxide solutions using potentiodynamic polarization.
2 Experimental Methods
Cathodic polarization measurements were performed using µAutolab system II, operated by GPES software with a scan rate of 5 mV/s from the open circuit potential. Moreover, the potential was started from open circuit potential (OCP) of approximately − 0.25 V moving to the more negative potential of − 2.0 V. The cell was a three-electrode all-glass cell, with a platinum counter electrode of dimensions 10 mm × 5 mm × 0.2 mm, and saturated calomel electrode was used as a reference electrode. Similarly, the electrochemical behaviour of Ni, Co and Ni–Co alloys was also investigated using the µAutolab system II with a scan rate of 10 mV/s, starting at 0 V and moved to anodic direction then it reversed to the cathodic direction. In addition, TTi Thurlby Thandar instrument PL310 (32 V-1A) PSU was used as the source of the direct current. Copper foils with a purity of 99.98% were utilized as a cathode (substrate), and a platinum mesh was the anode. The plating cell was a Pyrex cylinder of volume (1.2 L) with PTFE lid which contained five holes; these holes were utilized to insert the electrodes and thermometer.
Chemicals of Aldrich-Sigma grade were utilized in the electroplating baths such as NiSO4·7H2O, CoSO4·7H2O, H3BO3, sodium gluconate and cysteine. The chemicals were weighed and dissolved in deionized water, as shown in Table 1. The different concentrations of the chemicals were operated to optimize the electroplating of Ni–Co alloys. Also, sodium hydroxide (Aldrich grade) was utilized to study the electrochemical behaviour of Ni, Co and Ni–Co alloys.
The electroplating experiments of Ni, Co and Ni–Co alloys were performed via stagnant gluconate baths using a constant current density varied between 0.1 and 5 Adm−2. The electroplating time was one hour at 293 K on copper sheet. To stabilize the concentration of bath species, a fresh bath was prepared. Before each run, the copper substrate was etched in concentrated nitric acid (1:1) for 1 min to remove the oxides layer, then washed with deionized water, rinsed with acetone and weighed. The cathodic current efficiency was determined by weight measurement before and after the electroplating process. Electrochemical behaviour of the obtained Ni, Co and Ni–Co alloys was studied using potentiodynamic polarization in stagnant, naturally aerated sodium hydroxide solutions (0.01, 0.1, 1.0 M). Before each experiment, the working electrode was about 0.2 cm2 surface area to contact the solution. This working electrode was immersed quickly into the sodium hydroxide solution.
The surface morphology of the electroplated Ni, Co and Ni–Co alloys was examined by scanning electron microscopy (SEM) (JEOL JSM-5300 LV, at 25 kV under high vacuum). Furthermore, the chemical composition of the electroplated Ni–Co alloys was determined by energy dispersive X-ray analysis. The nanostructure of the Ni, Co and Ni–Co alloys was determined by X-ray diffraction with Philips X'Pert Pro Diffractometer, fitted with the X'Celerator and a secondary monochromator. To generate copper K-alpha radiation with a wavelength of 1.54 Å, a copper anode was supplied with a voltage of 40 kV and current of 0.04 A. The thickness of the electroplated Ni–Co alloys was determined using an optical microscope (OLYMPUS BX41 with Soft Imaging System).
3 Results and Discussion
3.1 Bath Characterization
Figure 1 illustrates the cathodic polarization curves performed using different electrolytes of Ni2+ or Co2+ and mixture of Ni2+ and Co2+ without and with different additives. The cathodic polarization curves displayed three growth region of cathodic current density which were a, b and c. During region a, reduction of Ni2+ to Ni+ occurred, this was proved by many researchers [3, 14]. In the region b, the reduction of Ni+ to Ni occurs and region c includes the hydrogen evolution reaction. The additives have a great effect on the reduction potential. Gluconate (baths 2) shifted significantly reduction potential of Ni2+ (regions a and b) to less negative values than Ni2+ (bath 1) which possesses very small reduction region, begun at − 0.9 V. Addition of boric acid as in bath 3 slightly moved the reduction potential of Ni than bath 2, to more positive value. Besides, the addition of cysteine (bath 4) shifted the reduction potential of Ni2+ to more positive values than that obtained by bath 1.
The electroplating potential of Ni2+ and Co2+ bath shifted gradually to a more positive value of − 1.175 V than that obtained using bath 1 as shown in Fig. 1b for baths 5, 6, 7 and 8. However, the shift of electroplating potential for the baths 10 and 11 was slightly moved to a more negative value of about − 1.19 V than bath 8. Comparing the cathodic polarization curve of the bath 4 of Ni2+ and bath 11 of Co2+, the electroplating potential of Ni2+ was slightly more positive than Co2+. Besides, region c shifted at potential about − 1.5 V which included sharply growth of cathodic current density due to reduction of H+.
The more positive shift of the reduction potential of Ni2+ and Co2+ due to the presence of the additives can be explained by the promotion of the initiation of Ni nucleation and delaying of the hydrogen reduction. The findings indicate that the addition of agents can effectively change and improve the microstructure and properties of the electroplated Ni–Co alloys. Sodium gluconate in the electroplating bath may act as a ligand for nickel ions leading to change in the film from burnt to white. These results are due to the formation of Ni–gluconate complex, which accelerates the transfer of electrons via ion bridging [3, 14] and which increases the rate of electroplating as can be seen from cathodic polarization measurements and lower the overpotential of Ni reduction reaction. Hydrogen evolution causes the formation of pits in coatings, but they were improved to less porous and granular grains by adding boric acid (anti-pitters). In fact, this effect could be due to the adsorption of boric acid species at the cathode which can minimize the effective surface available for proton reduction [15] and it is indicated by showing the more positive shift of electroplating potential of Ni or which enhance the reduction rate. The adsorption of Ni-boric acid complex species on the cathode may also lower the overpotential which is necessary for electroplating of Ni in sulphate solutions [16]. Therefore, boric acid increases the nucleation rate of Ni and Co as can be seen in Fig. 1.
Bright electrodeposited Ni–Co alloys were obtained by adding a brightening agent such as cysteine. The effect of cysteine can be attributed to its adsorption at the cathode surface; the adsorption of cysteine molecules at metal electrodes is related to the interaction of lone pair of electrons of –SH, –COOH and –NH2 groups with the Ni and Co ions and electrode surface as a ligand [14]. Cysteine follows non-blocking adsorption which occurs on the active sites of the crystal planes of the substrates and on the emerging surfaces of the crystallizing phases [17]. Therefore, cysteine can act as a hindrance and decelerate surface diffusion of adsorbed ions [18]. This causes more difficult grain growth and consequently higher nucleation rate, resulting in finer grains. Also, cysteine can form a complex with metal ions, increasing the number of formed complexes adsorbed on the electrode, and thus increase the rate of reduction (induced adsorption) or accelerating the rate of flow of electrons through the additive from the electrode to the metal ion (ion bridging) [3]. Cysteine supports similarly the electroplating of Ni and Co and due to shift of reduction potential to a more positive direction and small overpotential.
3.2 Morphology, Composition and Crystal Lattice of the Electroplated Ni–Co Alloys
Figure 2 shows the SEM images of electroplated Ni, Co and Ni–Co alloys obtained using a current density of 0.4 Adm−2 for 1 h at 293 K. The surface morphology of Ni was changed from burnt and porous to dense and shiny as shown in Fig. 2a–c. The additives included organic additives of sodium gluconate and cysteine and an inorganic additive of boric acid. The electroplated Ni obtained using bath 1 was burnt and porous. The slightly porous and granular Ni was obtained by addition of gluconate to the bath. Moreover, boric acid removes effectively pinholes, creates a granular coating. The presence of cysteine in the bath created dense and shiny Ni, as displayed in Fig. 2c. The surface morphology was dense for the Ni–Co alloys that contained a range of Co content between 1 and 45% such as Ni, Ni-17.68Co, Ni-34.81Co and Ni-42.44Co, as can be seen in Fig. 2c. However, with the rise of Co content in the Ni–Co alloys more than 45%, the micrograph revealed the spherical and nodular or coral reef-like structure of Ni-60.21Co, Ni-74.46Co, Ni-92.05Co alloys and Co, as can be seen in Fig. 2d–f. EDX analysis showed that electroplated Ni–Co alloys of different Co% were obtained from gluconate baths such as Ni-17.68Co, Ni-34.81Co, Ni-42.44Co, Ni-60.21Co, Ni-74.46Co Ni-92.05Co and Ni-97.36Co, as merged in Fig. 2 and Table 2.
Figure 3 displays XRD patterns of the electroplated Ni–Co alloys which displayed intensity peaks relating to nanocrystalline structures. The XRD patterns assured that Ni–Co alloys with Co % of 1–75% assembled in face-centred cubic (JCPDS number 35-1360) with unit cell parameters increase from a = 3.681 Å to a = 3.69 Å. Besides, the Ni–Co alloys with Co% more than 75% organized in hexagonal closed package HCP(JCPDS number 05-0727). The electroplated Ni, Ni-17.68Co, Ni-34.81Co, Ni-42.44Co, Ni-60.21Co, Ni-74.46Co alloys arranged in FCC lattice which possess lower interfacial free energy than HCP structures. Nonetheless, electroplated Ni-92.05Co and Co98.76% form HCP structures. Moreover, Nickel and cobalt are chemically and physically similar elements; because of the typical atomic size. Therefore, the electroplating of Ni and Co completely produces homogeneous alloys as a substitution solid solution [19]. The average grain size of the electroplated Ni–Co alloys coatings was calculated using Debye–Scherrer’s equation [20]: \(\tau = ({K\lambda})/({{\beta \cos \theta}})\) where λ is the X-ray wavelength, typically 1.54 Å, β is the line broadening at half the maximum intensity in radians, K is the shape factor, θ is the Bragg angle and \(\tau\) is the mean size of the ordered (crystalline) domains. The average grain size of Ni–Co alloys with Co% of 0–75% varied between 6.5 and 16.6 nm, while the average grain size of Ni–Co alloys with Co% of more than 75% varied between 20 and 22 nm.
Figure 4 shows the current efficiency of the electroplated Ni, Co and Ni–Co alloys which increased gradually with the increase of cobalt content. The lowest value of cathodic current efficiency was for Ni at nearly 66%. Moreover, the Ni-17.68Co, Ni-60.21Co, Ni-74.46Co and Ni-92.05Co alloys displayed the gradual increase of cathodic current efficiency of 71%, 72%, 73.9% and 75%, respectively. The highest current efficiency was obtained for pure Co, which was calculated about 75.8%. The thickness of coatings increased gradually with the increase of Co content in the alloys. The smallest thickness was obtained for Ni which is 14.61 µm. It was followed by Ni-17.68Co, Ni-60.21Co and Ni-74.46Co alloys, which were 17.71 µm, 26.19 µm, 27.94 µm and 27.72 µm, respectively, as shown in Fig. 4.
3.3 Potentiodynamic Polarization
Corrosion data were obtained using the potentiodynamic polarization curves as shown in Fig. 5 for electroplated Ni–Co alloys immersed in different concentrations of sodium hydroxide solution (0.01 M, 0.1 M and 1.0 M) at 293 K. The corrosion parameters were calculated using the Tafel extrapolation such as corrosion current density (icorr), corrosion potential (Ecorr), anodic Tafel slopes (βa) and (βc), as displayed in Table 3. The Electroplated Ni–Co alloys with high Ni% displayed low icorr but icorr is increased for Ni–Co alloys with high Co%. The electroplated Ni-17.68Co alloy possesses the lower icorr of 0.08 µA/cm2 in 0.01 M sodium hydroxide. However, the Ni-92.05Co alloy shows higher icorr of 3.5 µA/cm2 in 0.01 M NaOH solution. The icorr of the electroplated Ni–Co alloys increases with the increase of sodium hydroxide concentrations. The mixed corrosion potential, Ecorr, for the electroplated Ni–Co alloys shifted to anodic direction with the increase of sodium hydroxide concentrations. Figure 6 compares the variation of the corrosion rate Ni–Co alloys with the increase of Co content in 0.01 M, 0.1 M and 1.0 M NaOH solutions. The corrosion rate of the electroplated Ni–Co alloys in 0.01 M NaOH solution increased gradually from 0.00193 mm/year of Ni-17.68Co to 0.135 mm/year of Ni-92.05Co. However, the corrosion rate of pure Co decreased slightly than the corrosion rate obtained for Ni-92.05Co to 0.123 mm/year.
The corrosion rate of the electroplated Ni–Co alloys in 0.1 M increased gradually from 0.00503 to 0.398 mm/year with the increase of Co content. Moreover, the corrosion rate of the electroplated Ni–Co alloys in 1.0 M NaOH solution increased more sharply with the increase of Co content. Ni showed the lowest corrosion rate in 1.0 M which accounted to be 0.0279 mm/year, while Ni-92.05Co gave the highest corrosion rate in 1.0 M NaOH which was 0.909 mm/year.
The composition and morphological structure of the electroplated Ni–Co alloys has a great effect on their electrochemical behaviour in sodium hydroxide solutions. The low corrosion rate is obtained for electroplated Ni–Co alloys with low Co%, which can be due to the formation of Ni-hydroxide, Ni-oxide and Ni-oxyhydroxides as shown in Eqs. 1–5 [21]:
or [22]:
From Eqs. (1) and (2), water molecules adsorb at the working electrode surface and produce Ni hydroxide, which reacts with hydroxyl ion and forms oxyhydroxide. Also, hydroxyl ions can directly react with the metal surface and produce hydroxide and oxides. The stability of the formed layers on the surface of the coatings can be affected by increasing of Co content which can accelerate the dissolution of the layer leading to increase the icorr for Ni–Co alloys. Electroplated Ni and Ni–Co alloys with low Co% show generally the lowest rate of corrosion in sodium hydroxide solutions because of Ni-oxides and Ni-hydroxides. Ni-oxides and Ni-oxyhydroxides are stable which prevent continuous dissolution of Ni coating [23, 24]. However, the electroplated Ni–Co alloys with high Co% show high corrosion current densities and corrosion rate suggesting the continuous dissolution of oxyhydroxide layer. This is because cobalt is more active and susceptible to oxidation than nickel. Moreover, Tury et al. [21] revealed that the Co-based alloys produce no layer or a very thin layer, spongy oxide layer and porous CoOOH [25], causing the high dissolution rate [26]. Consequently, Co participates minimal effect in the formation of the protective film [27, 28]. In addition, the morphological structure or small grains of electroplated Ni–Co alloys with low Co% is dense and smooth which can lead to the formation of dense oxide/oxyhydroxide protective layer, which decreases the corrosion rate in NaOH solution. In contrary, the electroplated Ni–Co alloys with high Co% possess granular or spherical structure which can form non-dense or porous oxide/oxyhydroxide layer decreasing the formation of the protective layer which increases the corrosion rate.
4 Conclusion
The cathodic polarization measurements indicate that the gluconate, boric acid and cysteine shift electroplating potential of Ni and Co to less negative values and decrease the overpotential of Ni and Co reduction reaction enhancing the electroplating of the Ni–Co alloys. The surface morphology of electroplated Ni–Co alloys was changed from porous to dense and coral reef-like. Nanocrystalline Ni–Co alloys are obtained as a result of the addition of sodium gluconate, boric acid and cysteine that remove pores and produce lustrous or mirror-like coatings. The increase of Co Content led to the formation of a granular structure. The electroplated Ni–Co alloys with Co% of 0–75% arranged in FCC structure but the electroplated Ni–Co alloys with Co% more than 75% possessed HCP structure. Potentiodynamic polarization showed that electroplated Ni–Co alloys with low Co% possessed lower icorr and corrosion rate than electroplated Ni–Co alloys with high Co%.
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Authors acknowledge with thanks the financial supports granted by the Egyptian Cultural Bureau, the authors are grateful to the ACMA service at University of Newcastle, UK for SEM, XRD and EDX analysis.
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Negem, M., Helal, N., Roy, S. et al. Electroplating of Nanocrystalline Ni–Co Alloys Using Cysteine and Their Electrochemical Behaviour in NaOH Solution. J Bio Tribo Corros 6, 49 (2020). https://doi.org/10.1007/s40735-020-00346-x
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DOI: https://doi.org/10.1007/s40735-020-00346-x