Cathodic stripping voltammetry has been used for quantitative determination of ions which form sparingly soluble salts with anodically generated species. The insoluble salts are stripped cathodically to evaluate the charge which may be proportional to concentrations of the ions to be determined   . This technique has been applied to determine arsenic in sea water  , traces of telluriu  , aluminum, chromium and titanium  , nickel generated in sonoelectrochemistry  , tryptophan and histidine  , trace antimony  , cerium  , selenium in freshwaters  , iron in seawater   , titanium in seawater  , manganese  .
A key of stripping voltammetry lies in the equivalence between the stripped charge and the accumulated one which is proportional to concentrations of anionic analyte. The equivalence may not be ensured when 1) stability constants of the sparingly soluble salts are not large enough to be influenced by foreign species, 2) all the deposits are not electrochemically stripped owing to dispersion in a form of small particles to solution, and 3) the stripped charge includes capacitive charge. The first belongs to a chemical subject, and can be solved by selecting kinds of sparingly soluble salts. The second is a physical subject on uniform dissolution associated with the electric percolation  . If a part of the deposit near the electrode is dissolved more exceedingly than the other part near the solution, the latter loses an electric path to the electrode. As a result, it cannot be reduced electrochemically any more, and maybe dispersed to the solution in the form of salt particles, as illustrated in Figure 1. The loss of the electric path has been found in the reduction of electrically conducting polyaniline films    as well as polyaniline-coated latex particles  .
The third item involves techniques of subtracting capacitive currents. There are two sources of double layer capacitors, one being due to orientation of solvent dipoles   in Stern’s (inner) layer  , the other being to orientation of redox dipoles    . Since the latter is oriented in the opposite direction to the former, it shows negative values of the capacitance at high concentrations of redox species on the electrode. The deposit of insoluble species takes much higher concentration than the concentrations of diffusing redox species. Consequently, the effect of negative capacitance should contribute largely to the determination of the stripped charge.
This paper aims at evaluating a relationship between the accumulated charge and the negatively capacitive charge in cathodic stripping voltammetry of chloride ion in solution at a silver electrode. Silver chloride is deposited on the Ag electrode by a constant anodic voltage for a long time to evaluate the deposition charge. The charge does not include a capacitive component because of steady-state electrolysis. The cathodic charge is evaluated from integration of cathodically
Figure 1. Reduction of salt molecules on the electrode to make them electrical insulator, which interrupt the reduction of upper salt molecules.
scanned voltammograms, which is composed of the reduction charge and the negative capacitive charge. The capacitive charge is caused by the potential scan. Then the observed charge is different by the amount of capacitive charge. The negative capacitance at thick film will be shown to be cancelled with the double layer capacitive charge for dendrite formation.
All the chemicals were of analytical grade purchased from Nilaco (Tokyo), and were used as received. Water employed was distilled and then ion-exchanged. The working electrode was a silver wire 0.5 mm in diameter with 99.99% purity purchased by Nilaco (Tokyo). The electrode surface was polished with sand paper and then with 0.3 μm aluminum powder. The wire was inserted into solution by ca. 10 mm in depth with an optical stage. The accurate length of the immersion was determined from photographs. The usage of the wire instead of an inlaid disk prevented us from floating capacitance caused at the insulator|electrode boundary.
The reference electrodes were the Ag|AgCl electrode in saturated KCl solution, the Ag|AgxO electrode which was formed by immersing a silver wire in concentrated HNO3 for a few minutes, and the Ag|AgCl electrode directly inserted in a test solution. Although the second one and the last showed unstable equilibrium potentials for a long time measurement, they were helpful for avoiding leakage of chloride ion from the Ag|AgCl electrode. The unstable potential was corrected by use of Ag|AgCl (sat. KCl). All the potentials here were represented in terms of the potential at Ag|AgCl (sat. KCl). The counter electrode was a platinum coil. A potentiostat was CompactStat (Ivium, Netherlands).
All the solutions were deaerated with nitrogen gas for 20 min before each voltammetric run. The solution of the pH was adjusted to 3.0 by addition of HNO3. We have examined effects of pH of the solution for fear of formation of Ag(OH), but found no dependence on pH so far as pH less than 5.
3. Results and Discussion
Voltammograms in 0.1 M KNO3 at the Ag working electrode and the Ag|AgCl reference electrode showed the rising oxidation current and the peaked reduction wave, as shown in Figure 2(a). When the cell was left for an hour in the N2 atmosphere, a new oxidation and a reduction wave appeared at ca. 0.3 V and ca 0.2 V, respectively (Figure 2(b)). These waves are predicted to be caused by formation of AgCl with chloride ion leaking from the Ag|AgCl reference electrode. Since these waves were found by adding a small drop of KCl solution into the 0.1 M KNO3 solution, they can be obviously attributed to be the reaction AgCl + e− = Ag + Cl−. The behavior was also found by use of the saturated calomel electrode. Leakage of chloride ion has been significant in deionized latex suspensions  . Few attentions have been paid to the leakage although kinetic
Figure 2. Voltammograms in 0.1 M KNO3 at the Ag electrode observed (a) immediately after and (b) an hour after inserting the Ag|AgCl (sat. KCl) into the solution.
work on silver halides has a long term history for AgCl  , AgBr  and AgI   .
A test solution includes low concentrations of Cl−, which can work as a solution of a reference electrode just by inserting the AgCl-coated silver wire in the solution. This reference electrode exhibited such a stable equilibrium potential that cyclic voltammetric peak potentials of deposition and dissolution of AgCl did not change for a few hours under the deaerated AgNO3 solution. Unfortunately, these peak potentials varied slightly with bulk test solutions. We have confirmed that the peak potentials obeyed the Nernst equation for various concentrations, from which the shift of the potential by the AgCl-coated silver wire was estimated. All the potentials described here are the thus corrected values vs. Ag|AgCl (sat. KCl).
The anodic peak currents were proportional to not only v1/2 (v: potential scan rate), i.e. linear to v1/2 with the intercept of zero current, but also the concentration of Cl−. Therefore the anodic current should be controlled by diffusion of Cl−. We evaluated the diffusion coefficient of Cl− to be 1.48 × 10−5 cm2∙s−1 from these proportionality constants.
Potential 0.28 V was applied to the silver electrode in the deaerated 0.2 mM KCl + 0.1 M KNO3 solution to generate AgCl for a given period, and was anodically scanned, as shown in the right ordinate of Figure 3. The responding cathodic current was almost constant after 1 s (in the left ordinate of Figure 3) without noticeable charging current. The integration of the current yielded the oxidation charge, qo. In contrast, the reduction current increased rapidly with the linear potential scan, showed a peak, decreased drastically, and increased slightly with the time. The last increase may be caused by double layer (DL) charging current, because the linear increase in the capacitance can be explained by the electrically percolated silver and because the large current (−40 μA) can be interpreted as the DL capacitance of the percolated silver (ca. 1 mF∙cm−2). We eliminated the capacitive contribution indicated as the dashed line ((a) in Figure 3) from the reduction current, and evaluated the reduction charge, qr.
Figure 4 shows the variations of qo and −qr, against the oxidation time, to at
Figure 3. Current-time curve in the left axis in 0.2 mM KCl + 0.1 M KNO3 solution, and variation of the voltage with the in the right axis at v = 0.05 V∙s−1. Line (a) is a background current.
Figure 4. Variations of (circles) qo and (triangles) qr with the oxidation time, to, of the cathodic stripping in the solution (a) 0.4 mM KCl and (b) 2 mM KCl including 1 M KNO3 + 1 mM HNO3 at v = 0.05 V∙s−1 when the oxidation potentials were (a) 0.266 and 0.225 V vs. Ag|AgCl (sat. KCl).
given constant potentials. The proportionality of qo to to indicates some kinetic control of the oxidation rather than diffusion, and demonstrates to include no double layer charge, otherwise an intercept might appear  . Although qo should be compensated with qr, according to the conventional concept of the charge balance on the electrode, observed values of |qr| were always smaller than qo. The loss of the charge can be attributed to chemical complications such as dissolution of deposit AgCl, and items 2) and 3) described in Introduction. Firstly, we examine a possibility of chemical complications. If silver hydroxide or silver oxide is deposited electrochemically on the electrode, qr should be larger than the charge predicted from concentrations of Cl−. Acidic solutions (pH from 2 to 6) had no effect on the ratio, |qr|/qo, and hence silver hydroxide does not participate in the inequality (|qr| < qo). Silver ion diffusing in the bulk solution takes ca. 4 μM in 0.4 mM KCl solution. It cannot contribute to qr. There seems no possible chemical species of blocking the reduction.
In order to search unrecognized possibility of chemical contribution to the inequality, we carried out long-term double potential chronocoulometry. Application of a constant voltage generated the AgCl deposit, which was reduced by a constant potential. Figure 5 shows the dependence of the ratio of the oxidation
Figure 5. Variation of the ratio of the reduction charge at 0.005 V vs. Ag|AgCl (sat. KCl) to that of the oxidation one at 0.244 V by the double potential step chronoamperometry in the solution of 0.2 mM KCl + 0.1 M KNO3. Oxidation times ranged from 30 s to 270 s.
charge to the reduction one, |Qr|/Qo, on Qo. The ratios for −0.2 < log(Qo/μC) < 3.0 were unity, indicating the charges should be balanced. The difference in the variations between in Figure 4 and in Figure 5 should lie in the electrochemical techniques, i.e. the cathodic potential scan in Figure 4, which necessarily brings about the capacitive current. Therefore, the unbalance ought to be caused by the negative capacitance of redox reactions    . The decrease in the ratio for log(Qo/μC) > 3.0 may be caused by a loss of electric path for the reduction of AgCl by the percolation, as illustrated in Figure 1. The AgCl deposits for log(Qo/μC) = 0 and 3 have the densities of 6.5 × 10−11 and 6.5 × 10−8 mol∙cm−2, respectively, which correspond to 4 and 4000 AgCl molecules per nm2. Therefore, the point on the left in Figure 5 represents a monolayer, while that on the right does a thick film with more than 400 layers.
The negative capacitance can be represented by qo − |qr|. If it is caused only the redox reaction, values of qo − |qr| should be proportional to qo, or (qo − |qr|)/qo be a constant. Figure 6 shows variation of (qo − |qr|)/qo with log qo, obtained by change in concentrations of KCl and oxidation potentials. The prediction fails, the ratio decreasing with an increase in qo, although the proportionality of qo and qr with to was retained as in Figure 4(b). In anodic stripping voltammetry, the scanned potential for the deposited silver can oxidize the silver atoms at any location so far as they have electric connection to the electrode. In contrast, the reduction of an AgCl molecule in cathodic stripping voltammetry requires a contact with the electrically percolated silver atoms. Thus, it begins only at the substrate silver electrode, and then the reduction is propagated toward the film|solution interface. When percolated silver atoms grow in dendrite form, the surface of the dendrite works as an electrode of the cathodic stripping. As a result, the area of the silver|solution becomes much larger than the projected area of the electrode, as illustrated in the inset of Figure 6. Then the DL capacitance by the solvent dipoles should increase to compensate the negative capacitance, yielding the decrease in (qo − |qr|)/qo with the increase in the film thickness.
We estimate the dependence of the DL capacitance by the solvent dipoles at the dendrite|solution interface on qo. The silver atoms reduced from AgCl are
Figure 6. Dependence of the normalized negatively capacitive charge on the logarithms of the oxidation charge obtained for various values of oxidation potentials and in solutions of (triangles) 0.1 M KNO3 + 0.4 mM KCl + 1 mM HNO3, (circles) 0.1 M KNO3 + 0.4 mM KCl and (inverse triangles) 0.1 M KNO3 + 2 mM KCl + 1 mM HNO3. The inset illustrates silver dendrite (filled circles) around which the DL capacitor is formed.
necessarily adjacent to silver atoms, silver chloride molecules or water molecules, the last of which can generate the DL capacitance, C. Let the amount of the silver atoms on the electrode be w, which are electrically percolated to the electrode. C is a function of w, C(w). When a small amount of silver atoms, Δw, is generated by the electrode reaction, the capacitance is not formed only in the added amount, but should be formed over the whole silver atoms because of the electric percolation. It is all the percolated silver atoms that can compensate the increment by the reduction. Thus, the increment of the capacitance is proportional to (Δw)/w rather than Δw. As a result we have
C(w + Δw) − C(w) = k (Δw)/w (1)
where k is a proportional constant. The Taylor expansion, C(w + Δw) = C + (dC/dw)Δw + ..., leads Equation (1) to dC/dw = k/w. The integration on the condition of C = 0 at w= w0 yields
C = k ln(w/w0) (2)
Since w is equivalent to qr, it should be proportional to qo. Therefore, the DL capacitance has the linear relation with log qo. This contribution is equivalent to the inverse triangle in Figure 6. Consequently, the observed reduction charge varies linearly with log qo.
From Figure 6, this value is close to the experimental one for log(qo/μC) ® 0, corresponding to a monolayer. A half the faradaic charge is consumed by the negative capacitance. When cathodic stripping is applied to quantitative determination of anions in solution, a calibration curve is predicted to be not linear but to exhibit low deviation from the calibration line at lower concentrations.
The negative capacitance is involved in the cathodic stripping voltammograms so that the reduction charge is smaller than the deposited charge. When the amount of the deposit is close to a monolayer, the reduction charge is half of the oxidation one because of the negative capacitive charge by the redox reaction. In contrast, deposits with as high as 10−7 mol∙cm−2 provide apparently the reduction charge equivalent to the oxidation one. However, the similarity of the charges is not due to the reversible redox reaction, but is ascribed to the compensation of the negatively capacitive charge with the DL charge by solvent dipoles.
The ratio |qr|/qo varies with values of qo, and hence a calibration curve for quantitative determination of anions does not take a line. It is dangerous to extrapolate the calibration line to zero concentration. Evaluated concentration may be overestimated.
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