D824 Journal of The Electrochemical Society, 161 (14) D824-D830 (2014) 0013-4651/2014/161(14)/D824/7/$31.00 © The Electrochemical Society The Electrodeposition of Lead in LiCl-KCl-PbCl2 and LiCl-KCl-PbCl2 -PbO Melts P. Pershin,a Yu. Khalimullina,a P. Arkhipov,a,z and Yu. Zaikova,b a Institute of High Temperature Electrochemistry, 620990 Yekaterinburg, Russia b Ural Federal University named after the first President of Russia B. N. Yeltsin, 620002 Yekaterinburg, Russia The mechanism for the electrode process that occurs on a molybdenum substrate in LiCl-KCl-PbCl2 and LiCl-KCl-PbCl2 -PbO melts depending on the concentration of PbO was investigated over the temperature range of 723–823 K using stationary polarization curves and voltammetry techniques. An increase in the concentration of PbO was found to decrease the diffusion-limiting current density for the recovery of lead, which was identified by the appearance of an additional peak in the voltammograms; it can be explained by a decrease in the concentration of Pb2+ ions decrease due to the formation of Pb2 O2+ complex ions in the electrolyte. The evaluation of the equilibrium constant KE and the rate constant of the reaction suggests that this reaction is strongly shifted toward the formation of the Pb2 O2+ complex ions. A theoretical polarization curve for the diffusion kinetics was calculated. © 2014 The Electrochemical Society. [DOI: 10.1149/2.0051501jes] All rights reserved. Manuscript submitted August 19, 2014; revised manuscript received October 3, 2014. Published October 31, 2014. Investigating the kinetics of electrode processes allows one to determine the kinetic parameters of reactions, to calculate the activation energies of these reactions and to establish the limiting stages of electrode processes.1 Additionally, data related to the mechanism of the electrode processes is valuable for developing the scientific basis for electrochemical technologies that meet the current ecological and energy saving requirements. In the literature, considerable attention is focused on the electrorecovery of lead from molten salts. The authors2,3 reported that the electro recovery of Pb2+ ions from a LiCl-KCl melt is a diffusioncontrolled, single-stage reaction. Haaberg et al.4 investigated the lead electrodeposition process in LiCl-KCl melts and in pure PbCl2 and determined that the migration of Pb2+ ions controls the rate of the cathode process in the pure PbCl2 melt at temperatures from 823 to 858 K. A diffusion regime of the process was observed in the LiCl-KCl melt; the diffusion coefficient for the Pb2+ ions was equal to 2 · 10−5 sm2 /s. The cathode behavior of lead ions on a molybdenum substrate in LiCl-KCl-PbCl2 and LiCl-KCl-PbCl2 -MgCl2 melts was studied using voltammetry and chronopotentiometry techniques in later works.5 The extraction of lithium from the initially deposited lead was found to result in the formation of a Li-Pb alloy in LiCl-KCl-PbCl2 and LiPb-Mg melts with the addition of MgCl2 . The diffusion coefficient of Pb2+ ions was determined using various techniques, and its value was found to be 2.26 · 10−5 sm2 /s. In a number of studies, there are considerable differences regarding the mechanism of the cathode process. Therefore, Strenberg et al.6 established a two-stage mechanism for the recovery of Pb2+ ions through the stage of the formation of monovalent Pb+ ions. These works were primarily performed during the second half of the XXth century and were related to dilute solutions of lead in alkali metal chlorides, free of oxide ions. There is no information available regarding the mechanisms of electrode processes in oxide-chloride melts. The structures and compositions of ionic melts affect the electrode processes that occur during the production and refining of metals via the electrolysis of chloride melts. The oxide admixtures introduced into the melt together with the raw material significantly change the melt structure due to the formation of oxide-chloride complexes. The experimental results allow the regularities of the cathode process to be established and the structures of the ionic groups in the oxide-chloride melts to be defined. The objective of the present work is to study the mechanism and kinetics of the electrode reactions during the recovery of lead ions fromLiCl-KCl-PbCl2 and LiCl-KCl-PbCl2 -PbO melts. z E-mail: [email protected] Experimental Experimental cell.— The cathode processes in LiCl-KCl-PbCl2 and LiCl-KCl-PbCl2 -PbO melts were investigated using stationary galvanostatic polarization curves and voltammetry techniques. An IPC-Pro potentiostat (VoltaProm LLC, Saint-Petersburg, Russian Federation) and an AutoLab PGSTAT 302N galvanostat-potentiostat (Metrohm Autolab B.W. Utrecht, the Netherlands) were used to record galvanostatic impulses and responses. An APPA-109 N multimeter (Appa Technology Corporation, Taiwan) was used as an additional recording device. A schematic of the experimental electrochemical cell is presented in Figure 1. The experiments were carried out in a quartz tube 3, which was hermetically sealed with a fluoroplastic cover 2 that contained openings for electrodes and a thermocouple. An alundum crucible 10 was placed at the bottom of the cell on a special support composed of heat-resistant bricks 15. Metallic lead 14 and the prepared electrolyte 11 were loaded into the crucible, and then the reference electrode 7, working electrode 6 and alundum sheath 8 with a thermocouple 9 were installed. A molybdenum rod in an alundum tube-case served as the working electrode (cathode). The electrode area was chosen in such a way that the electrode length / the electrode diameter ratio to be more than 10. Thus, the molybdenum rod length was 17 mm, its diameter was 1 mm and the total surface area was 0.54 cm2 . Molybdenum was selected as the material for the working electrode because it does not interact with lead under the experimental conditions. Other materials, such as graphite and glassy carbon, could not be used as electrode materials because of the possibility to recover PbO to metallic lead. Metallic lead placed at the bottom of the alundum crucible was used as an auxiliary electrode. The measurements were performed relative to the liquid lead 13 contacting the melt of the same composition. A molten eutectic mixture of lithium and potassium chlorides (45–55 mol.%) with added lead oxide and lead chloride was used as the electrolyte for both the auxiliary and the working electrodes. The testing electrolyte and the reference electrode electrolyte were separated by the diaphragm of the Gooch asbestos crucibles 12. Molybdenum rods 5, which were protected from contact with the melt by alundum tubes 4, were used as the current leads to the liquid metal electrodes. The free ends of the current leads were covered with rubber plugs 1 to keep the cell hermetically sealed. The cell was hermetically sealed, evacuated and filled with purified, dried argon. Then, the cell was placed into a resistance furnace and heated to the desired temperature under excess argon pressure. The assembly was equipped with an automatic temperature stabilizing system, which controlled temperature fluctuations within ± 2◦ . A Chromel-Alumel thermocouple 9 was used to measure the temperature of the cell. Downloaded on 2016-03-06 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract). Journal of The Electrochemical Society, 161 (14) D824-D830 (2014) D825 Lithium chloride (chemically pure grade), potassium chloride (chemically pure grade), lead chloride (analysis grade) and PbO (ultrahigh purity) were used to prepare the electrolyte (Closed Joint-Stock Company “Khimreactivsnab”, Ufa, Russian Federation). Metallic lead (purity of 99.985, Ural Mining Metallurgical Company, V. Pyshma, Russian Federation) was used for the reference and auxiliary electrodes. Preparation of salts and electrolyte.— Potassium chloride was dried under vacuum at 673 K and then melted under an argon atmosphere. Lithium chloride was dried in a glassy carbon crucible, first at 473 K and then at 673 K, and then it was melted at 973 K under an argon atmosphere. The prepared KCl and LiCl salts were mixed in a 0.55–0.45 molar ratio and melted at 723 K under an argon atmosphere. Lead chloride was dried at 473 K and purified using the zone-melting method. Lead (II) oxide was dried under vacuum at 473 K. The salts were stored in a glove box under a dry atmosphere. For each experiment, 100 g of the prepared salt mixture was used. The appropriate salts and oxide samples were weighed on a Shimadzu BL-220H (Shimadzu Corporation, Kyoto, Japan) balance with an accuracy of 0.001 g. Results Figure 1. Schematic of the experimental cell: 1 – Rubber plugs; 2 – Fluoroplastic cover; 3 – Quartz test tube; 4 – Alundum tubes; 5 – Current leads to electrodes; 6 – Working electrode (Mo); 7 – Reference electrode quartz sheath; 8 – Thermocouple sheath; 9 – Thermocouple; 10 – Alundum crucible; 11 – Electrolyte; 12 – Gooch asbestos crucible; 13 – Reference electrode (Pb); 14 – Counter electrode (Pb); 15 – Heat-resistant brick support. Stationary galvanostatic polarization curve technique.— The lead electrodeposition process in the LiCl-KCl-PbCl2 melt on a molybdenum substrate was investigated at temperatures from 723 to 823 K and lead chloride concentrations of 1.06 and 2.10 mole%. During the experiment, the overvoltage values were determined at the moment of steady-state current shutdown in galvanostatic mode. The polarization curves are presented in Figure 2. An insignificant deviation in the potential from its equilibrium value was observed in the initial area of the polarization curves as the cathode current density increased to 0.4 A/cm2 (Fig. 2B). The dependency of η on lg(1-i/id ) is presented on Figure 3. The experimental points in the [η – lg(1-i/id )] coordinates remained within the straight lines. The tangent of the inclination angle is equal to tgα = 0.032, 0.034 and 0.036 V. Figure 2. Polarization curves for the recovery of Pb2+ ions from the LiCl-KCl-PbCl2 melt: A: Temperature dependency at a PbCl2 concentration of 1.06 mole%; B: Temperature dependency at a PbCl2 concentration of 2.10 mole%; C: Concentration dependency at 723 K. Downloaded on 2016-03-06 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract). D826 Journal of The Electrochemical Society, 161 (14) D824-D830 (2014) Figure 3. Dependence of n on lg(1-i/1d ): A – 723 K; B – 773 K; C – 823 K. Table I. Values of the limiting current density (id , A/cm2 ) for the electrodeposition of lead ions in the LiCl-KCl-PbCl2 melt. CPbCl2 , mole% T, K 723 773 823 1.06 2.10 0.220 0.520 0.335 0.700 0.480 0.900 The number of electrons participating in the electrode reaction was obtained according to equation 1: n= RT tgα · F [1] Values of n = 2.00, 1.96 and 1.97 were calculated for temperatures 723, 773 and 823 K, respectively. The cathode reaction can be described as follows: Pb2+ + 2e → Pb0 [2] When the current density reached values of 0.184, 0.323 and 0.406 A/cm2 at 723, 773 and 823 K, respectively (Fig. 2B), a sharp negative shift in the potential to values of −1.003, −1.284 and −1.316 V was observed. The diffusion-limiting current density for the recovery of lead increased with temperature and the concentration of PbCl2 (Fig. 2). At a PbCl2 concentration of 1.06 mole% and temperature of 723 K, the limiting current density was equal to 0.220 A/cm2 , and at the same PbCl2 concentration and temperatures of 773 K and 823 K, the limiting current densities were 0.335 and 0.480 A/cm2 , respectively. When the PbCl2 concentration increased to 2.10 mole%, the limiting current density increased to 0.520 A/cm2 at 723 K. The id values are presented in Table I. The analysis of the obtained dependences and literature data2–6 revealed the diffusion nature of the limiting current density for the recovery of lead. At the negative potential shift to −1.0 ÷ −1.3 V (relative to the lead reference electrode), the recovery of lithium ions (Li+ ) occurs according to the following reaction: Li+ + e = Li◦ [3] The low potential values for the recovery of alkali metal can be explained by the formation of a lead and lithium alloy. Zhang et al.5 reported that PbLi3 and Li7 Pb2 compounds may be formed at the cathode surface in the LiCl-KCl-PbCl2 melt. The polarization curves for the electrode process in the LiCl-KClPbCl2 -PbO melt as a function of the lead (II) oxide concentration and temperature are given in Figure 4. Figure 4. Polarization curves for the recovery of Pb2+ ions from the LiCl-KCl-PbCl2 -PbO melt with a lead chloride concentration of 2.10 mole%: A: Dependence on the PbO concentration at 773 K; B: Dependence on the PbO concentration at 823 K; C: Temperature dependency at a PbO concentration of 1.20 mole%. Downloaded on 2016-03-06 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract). Journal of The Electrochemical Society, 161 (14) D824-D830 (2014) D827 Table II. Values of the limiting current density (id , A/cm2 ) for the electrodeposition of lead ions in the LiCl-KCl-PbCl2 -PbO melt at a PbCl2 concentration of 2.10 mole%. CPbO , mole% T, K 723 773 823 0.00 0.54 1.20 1.78 0.520 0.330 0.200 0.125 0.700 0.520 0.280 0.160 0.900 0.580 0.360 0.220 This figure clearly indicates that the dependences [i – η] have a similar form as the curves obtained in the melts without lead oxide (Fig. 2). However, the limiting current density values in the oxidechloride melts are considerably lower than in chloride melts. The initial area of the polarization curves shows an increasing cathode current density and an insignificant deviation in potential from the equilibrium value. The values of tgα for the [η – lg(1-i/id )] dependency are 0.031,0.033 and 0.036 V at 723, 773 and 823 K, respectively. The number of electrons calculated according to equation 1 is equal to n = 2.00, 2.02 and 1.98. The form of the polarization curves and their temperature and PbO concentration dependences indicate that the cathode reaction is a diffusion-controlled process. The values of the limiting current densities for the electrodeposition of lead (II) ions in the LiCl-KClPbCl2 -PbO melt are presented in Table II. From the diffusion kinetics perspective, the diffusion-limiting current density should increase as the concentration of potential-forming ions increases. However, the plot (Fig. 4) indicates that the diffusionlimiting current density for the recovery of lead ions in the oxidechloride melt is considerably lower than that in the pure chloride melt under otherwise equal conditions. The addition of PbO to the chloride melt results in a decreasing limiting current density for the electrochemical recovery of lead ions. This fact has never been mentioned in the literature. This phenomenon is apparently associated with the physical and chemical properties of the melt and its changes. Voltammetry.— The electroreduction of lead (II) ions on a molybdenum substrate in LiCl-KCl-PbCl2 melts with lead chloride concentrations of 1.06 and 2.10 mole% and in LiCl-KCl-PbCl2 -PbO melts with a lead chloride concentration of 2.10 mole% and lead oxide concentrations of 0.54, 1.20 and 1.78 mole% were studied using cyclic Figure 5. Cyclic voltammograms for a Mo electrode in LiCl-KCl at 773 K with various scan rates: 1–0.2 V/s; 2–0.1 V/s; 3–0.05 V/s. voltammetry over the temperature range of 723–823 K and sweep potential range of 50–650 mV/s. The range of potentials was selected bytaking into account the investigation of only the cathode process (from zero to −1.4 V relative to the lead reference electrode) because the molybdenum rod will dissolve in the anode region of potentials. The impossibility of using graphite and glassy carbon in our experiments was mentioned above. The background voltammograms in the LiCl-KCl melt at 773 K (Fig. 5) confirm the purity of the studied electrolyte. In the potential range from 0–1.0 V, no peaks were observed, and further shifting of the potential leads to the recovery of lithium ions (Li+ ) according to reaction 3. Figure 6 presents the LiCl-KCl-PbCl2 voltammograms depending on the temperature and potential sweep rate within the range from 0.10 to 0.65 V/s. When the potential sweep shifts to the cathode side, only one electroreduction peak of the lead ions is observed at all potential sweeps, as described by reaction 2 for the recovery of lead. The number of electrons participating in the cathode process was calculated according to equation valid only for reversible processes:7 E P/2 − E p = 2.20 · RT , nF [4] Figure 6. Cyclic voltammograms for a Mo electrode in a LiCl-KCl-PbCl2 (1.06 mole%): A: At 823 K with various scan rates: 1–0.1 V/s; 2–0.2 V/s; 3–0.5 V/s; 4–0.65 V/s. B: Under a potential sweep rate of 0.10 V/s at different temperatures: 1–723 K; 2–773 K; 3–823 K. Downloaded on 2016-03-06 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract). D828 Journal of The Electrochemical Society, 161 (14) D824-D830 (2014) Figure 7. Dependence of the peak current on the square root of the sweep rate in a LiCl-KCl-PbCl2 melt on a Mo electrode at 823 K at a PbCl2 concentration of 2.10 mole%. where Ep - peak potential; EP/2 - half-peak potential; F - Faraday constant, 96484 C/mole; R - absolute gas constant, 8.314 J/mole; T - temperature, K; n - number of electrons. Thus, the average value of the number of electrons for the cathode process was determined to be 1.97 ± 0.04. The study of the peak potential dependency on the logarithm of the sweep rate revealed that the peak potential insignificantly shifts to the cathode side, from −124 to −129 mV, as the sweep rate increases. This result indicates that the reduction of lead ions in the LiCl-KCl-PbCl2 melt is a reversible process.5 The Ip – V1/2 dependency (Fig. 7) is a continuous straight line that is extrapolated through the origin of the coordinates. The obtained results confirm that the electroreduction of Pb2+ in the chloride melt is controlled by diffusion throughout the potential sweep range under the experimental conditions. The diffusion coefficient for the lead ions in the LiCl-KCl-PbCl2 melt was calculated as described by the Berzins-Delahay equation:5,8 n F 1/2 1/2 1/2 I p = 0.61 · n F SC D V , [5] RT where Ip - cathode current peak, A; V - potential sweep rate, V/s; S - cathode area, cm2 ; D - diffusion coefficient, cm2 /s; C - concentration of electroactive particles, mole/vm3 . The calculated values of the diffusion coefficients for the Pb2+ ions in the LiCl-KCl-PbCl2 melt are 1.91, 2.29, and 2.59 · 10−5 cm2 /s at 723, 773 and 823 K, respectively. These values are in good agreement with the literature data.3,9 The obtained results confirm that the reduction of Pb2+ ions on the Mo substrate in the LiCl-KCl-PbCl2 melt over the temperature range of 723–823 K is a one-stage diffusion-controlled reaction. Figure 8 presents voltammograms for the LiCl-KCl-PbCl2 -PbO (1.78 mol.%) melt at 823 K depending on the potential sweep rate within the range from 0.25 to 0.65 V/s. Two peaks are observed in the voltammograms of the cathode process when PbO is added to the LiCl-KCl-PbCl2 -PbO melt. Figure 8. Cyclic voltammograms for a Mo electrode in a LiCl-KCl-PbCl2 PbO (1.78 mole%) melt at 823 K with various scan rates: 1–0.25 V/s; 2–0.35 V/s; 3–0.45 V/s; 4–0.55 V/s; 5–0.65 V/s. hypothesize that the addition of lead (II) oxide to the LiCl-KCl-PbCl2 melt results in the following equilibrium: PbCl2 + PbO ↔ Pb2 OCl2 [6] We previously studied the thermodynamic properties of dilute PbO solutions in the KCl-PbCl2 melt.12 These systems were found to have a negative deviation from Raul’s law. Such behavior was explained by the formation of complex compounds, particularly Pb2 OCl2 . From analysis of the voltammograms in the LiCl-KCl-PbCl2 -PbO (Fig. 8) melt, we conclude that the cathode process can be viewed as the reduction of two different electroactive ions at different potential values. Cathode peak A corresponds to the reduction of lead ions, as described by equation 2. The peak value increases according to the module as the sweep rate increases, and the potential peak value shifts to the cathode area. Cathode peak B is related to the reduction of the Pb2 O2+ oxide complex formed as a result of the interaction of lead oxide with the chloride melt.11 This process is the electrochemical reaction for the reduction of lead with the preliminary chemical decomplexation reaction. Therefore, the total electrode reaction for peak B may be described as follows: Pb2 O2+ + 2e → PbO + Pb0 1/2 [7] 2+ The Ip/V dependences for the electroreduction of Pb and Pb2 O2+ ions in the oxychloride melts (Fig. 9) are linear, i.e., the limiting stage is constant throughout the sweep rate range. Discussion Previous works10,11 have reported that if PbO is added to the leadcontaining melt, the formation of the Pb2 OCl2 compound is thermodynamically possible. The X-ray phase analysis also showed the presence of the Pb2 OCl2 compound in the frozen electrolyte. Therefore, based on the analyses in the above-cited works, it is possible to Figure 9. Dependence of the peak current B on the square root of the sweep rate in a LiCl-KCl-PbCl2 -PbO melt at 823 K. Downloaded on 2016-03-06 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract). Journal of The Electrochemical Society, 161 (14) D824-D830 (2014) D829 complex compound: N Pb2 OCl2 = N PbO [9] 2+ particles that participate The concentration of electroactive Pb in the electrode process is equal to: 0 − N Pb2 OCl2 N Pb2+ = N PbCl 2 [10] 0 where N PbCl2 – the initial molar fraction of PbCl2 . The molar fraction was then recalculated to the molar concentration according to the equation: C Pb2+ = N Pb2+ · ρ LiCl−K Cl−PbCl2 μ LiCl−K Cl−PbCl2 [11] where ρLiCl-KCl-PbCl2 – density of LiCl-KCl-PbCl2 , g/cm3 ;13 μ LiCl-KCl-PbCl2 – molar mass of LiCl-KCl-PbCl2 , g/mole. Figure 10. Voltammograms from the LiCl-KCl-PbCl2 -PbO melt at 823 K with different concentrations of PbO at a PbCl2 concentration of 2.10 mole%. The increasing concentration of PbO in the LiCl-KCl-PbCl2 -PbO melt caused the absolute magnitude of the peak A current to decrease, which corresponds to the lead electroreduction according reaction 2 under otherwise equal conditions. The increase in the peak B current corresponds to an increase in the PbO concentration in the melt, and the peak A current simultaneously reflects a decrease in the concentration of Pb2+ electroactive ions (Fig. 10). This result confirms the hypothesis that the lead oxide (II) forms Pb2 O2+ oxychloride complexes while interacting with the chloride melt. The KE constant of equilibrium (6) was calculated according to the equation: −G [8] KE = ex p RT where KE – constant of equilibrium; G – the Gibbs energy of the equation 6; The values for the KE constant are 74.34, 40.61 and 23.50 for 773, 823 and 873 K, respectively. These high values of KE assume that equilibrium (6) is almost completely shifted toward the formation of the Pb2 OCl2 complex compound. This fact also can be confirmed with the linear dependency of id as a function of difference of molar fractions of PbCl2 and PbO (Fig. 11). Based on the previous discussion, we can conclude that the equilibrium (6) will be significantly shifted toward the formation of the Pb2 OCl2 compound in the studied LiCl-KCl-PbCl2 -PbO melt. In this case, the molar fraction concentration of the dissolved lead oxide can be considered as the concentration of the formed Pb2 OCl2 Figure 11. Dependence of id on the molar fraction of PbCl2 and PbO difference in a LiCl-KCl-PbCl2 -PbO melt at 773 K. At high values of KE the value of the registered current will be proportional to the equilibrium concentration of the lead ions. The nature of this current will be defined by diffusion. The curve equation for the equilibrium conditions of the polarization will be written as follows: zF ·η , [12] i = id · 1 − exp RT where id - limiting diffusion current density, A/cm2 ; n - number of electrons; F - Faraday’s constant, 96485 C/mole; R - ideal gas constant, 8.314 J/(mole · K); T - temperature, K; n - overvoltage, V. The diffusion-limiting current density is determined according to the following equation: id = n F D Pb2+ C Pb2+ , δ [13] where, DPb2+ - diffusion coefficient of the lead ions, cm2 /s; SPb2+ - concentration of the electroactive lead ions, mole/cm3 ; δ - thickness of the diffusion layer. Experimental determination of the diffusion layer thickness in the conditions of “natural” convection for laboratory electrolyzers where halide fusions were exposed to electrolysis, represent a values of δ within 0.5 mm.14 For equation 13, the value of DPb2+ , calculated from voltammetry data using Berzins-Delahay equation, equal to 2.29 · 10−5 cm2 /s for the temperature of 773 K was used. Thus, the final equation for the polarization curve can be presented as follows: nF n F D Pb2+ C Pb2+ · 1 − exp · . [14] i= δ RT The comparison of the polarization curve for electrorecovery of lead ions in the LiCl-KCl-PbCl2 -PbO melt at a PbCl2 concentration of 2.10 mole%, PbO concentration of 1.20 mole% and temperature of 773 K with the polarization curve calculated according to expression (14) is presented in Figure 12. This figure demonstrates that the experimental data and calculated polarization dependency are in good agreement, and the calculated curve is slightly above the experimental one only in the current density range from 0.3 to 0.5 A/cm2 . Deviations of an experimental curve from theoretical one probably connected with lower values of diffusion coefficient of lead-containing oxide ions in comparison with diffusion coefficient of lead (II) ions in the same electrolyte. Besides the formation of lead-containing oxide ions12 can increase thickness of a diffusion layer, that also leads to decrease of current density. Downloaded on 2016-03-06 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract). D830 Journal of The Electrochemical Society, 161 (14) D824-D830 (2014) 2. 3. 4. ode process in LiCl-KCl-PbCl2 and LiCl-KCl-PbCl2 -PbO melts within the temperature range of 723–823 K. The increase in the concentration of PbO in the electrolyte is determined to reduce the diffusion-limiting current density for the electrodeposition of lead. The decrease in the diffusion-limiting current density appears to be due to the reduced concentration of free Pb2+ ions resulting from the formation of the Pb2 O2+ ions in the electrolyte. One current peak corresponding to the recovery of Pb2+ ions in the LiCl-KCl-PbCl2 melt is observed. It is shown that the recovery of lead (II) ions in the chloride melt is eversible and diffusion-controlled process. The introduction of PbO into the LiCl-KCl-PbCl2 melt leads to the appearance of a second current peak in the voltammograms. The additional cathode peak is related to the reduction of the Pb2 O2+ oxide complex that formed as a result of the interaction of lead oxide with the chloride melt. Acknowledgment Figure 12. Polarization curves for the recovery of Pb2+ ions from a LiClKCl-PbCl2 -PbO melt with a lead chloride concentration of 2.10 mole% and lead oxide concentration of 1.20 mole% at 773 K: Solid line - experimental dependency; Dotted line - calculated dependency. Thus, the addition of lead oxide to the lead chloride-containing melt complicates the electrode process due to the formation of the complex ion: PbO + Pb2+ → Pb2 O2+ [15] The evaluation of the equilibrium constant KE and the rate constant of reaction15 allows one to observe that this reaction is strongly shifted to the right toward the formation of the Pb2 O2+ complex ions. In this case, the registered current has diffusion character and is defined by the equilibrium concentration of free Pb2+ ions. Conclusions 1. Stationary galvanostatic polarization curves and voltammetry techniques were used to investigate the mechanism for the cath- The authors gratefully acknowledge the Shared Access Centre “Composition of Compounds” for analytical support. This work was financially supported by the Russian Federation President Grant MK-5678.2014.3. References 1. V. N. Nekrasov, A. V. Suzdaltsev, O. V. Limanovskaya, A. P. Khramov, and Yu. P. Zaikov, Electrochim. Acta, 75, 296 (2012). 2. E. Smidt, Electrochim. Acta, 8, 23 (1963). 3. V. P. Yurkinskiy and D. V. Makarov, J. of appl. chem. 67, 1283 (1994). 4. G. M. Haarberg, L. E. Owe, B. Qin, J. Wang, and R. Tunold, ECS Transactions, 50, 215 (2012). 5. M. Zhang, L. Chen, W. Han, Y. Yan, and P. Cao, Transactions nonferrous metals society. China, 22, 711 (2012). 6. S. Strenberg, T. Visan, N. Bonciocat, and A. Cotârtâ, Revue roumaine de chimie, 32, 883 (1987). 7. Z. Galus, Electrochemical analysis theoretical bases. Moscow, Mir (1974). 8. Y. Castrillejo, S. Palmero, M. A. Garcı́a, L. Debán, and P. Sanchez Batanero, Electrochim. Acta 41, 2461 (1996). 9. R. J. Heus and J. J. Egan, J. Electrochem. Soc. 107, 824 (1960). 10. H. Sugavara, K. Nagata, and K. S. Goto, Metallurg. Trans. 8B, 511 (1977). 11. S. N. Flengas and A. Hacetoglu, Can. J. Chem. 68, 236 (1990). 12. P. S. Pershin, V. P. Batukhtin, N. I. Shurov, P. A. Arkhipov, and Yu. P. Zaikov, J. Chem. Eng. Data, 57, 2811 (2012). 13. G. Liu, T. Utigard, and J. M. Toguru, J. Chem. Eng. Data, 31(3), 342 (1986). 14. A. N. Baraboshkin, Electrocrystallization of metals from molten salts. Moscow: Science, 280 p. (1976) (in Russian). 15. P. S. Pershin, A. A. Kataev, N. I. Shurov, P. A. Arkhipov, and Yu. P. Zaikov, Russian journal of Non-Ferrous Metals, 54, 195 (2013). Downloaded on 2016-03-06 to IP 130.203.136.75 address. Redistribution subject to ECS terms of use (see ecsdl.org/site/terms_use) unless CC License in place (see abstract).
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