Polarographic Coefficients of Some Elements in the Method of Amalgam Polarography with Accumulation

M. S. ZAKHAROV, A. V. KONKOVA
Submitted 1967 | SovietRxiv: ru-196701.09890 | Translated from Russian

Abstract Generated abstract

This study determines standard polarographic coefficients for elements analyzed by amalgam polarography with accumulation in several commonly used supporting electrolytes. Using previously defined coefficients for stirring, electrolysis, sensitivity, peak shape, attenuation, and concentration, the authors report mean experimental values from repeated measurements for elements including copper, lead, cadmium, zinc, and thallium in chloride, fluoride, acetate, ammonia, and tartrate media. The results show substantial variation by element and supporting electrolyte, reflecting differences in analytical sensitivity, diffusion behavior in mercury, and the reversibility of electrode processes. Comparisons such as those for zinc indicate that these coefficients can be used to evaluate favorable media for determination and to characterize anodic and cathodic wave behavior.

Full Text

POLAROGRAPHIC COEFFICIENTS OF SOME ELEMENTS IN THE METHOD OF AMALGAM POLAROGRAPHY WITH ACCUMULATION

Communication II

M. S. ZAKHAROV, A. V. KONKOVA

(Presented by the scientific-methodological seminar of the CTF)

As is known, for one and the same element on different supporting electrolytes and under different hydrodynamic conditions during the accumulation of the substance in the mercury electrode, and at different pH values of the solution, anodic waves may be obtained that differ in shape, depth, etc. In connection with this, to characterize anodic waves, cathodic peaks, and the electrolysis current, in works [1, 2] a number of coefficients were proposed: \(\gamma_{\mathrm{p}}^{0}\), \(\gamma_{\mathrm{e}}^{0}\), \(\gamma_{\mathrm{ch}}^{0}\), \(\gamma_{\mathrm{f}}^{0}\), \(\gamma_{0}^{0}\), \(\gamma_{\mathrm{k}}^{0}\)—the coefficients of stirring, electrolysis, sensitivity, shape, attenuation, and concentration under standard conditions \((t = 25^\circ\mathrm{C}, w = 10^{-2}\ \mathrm{V/sec};\ K_1 = 500z\ \mathrm{a\cdot cm\cdot mole}^{-1})\):

\[ \gamma_{\mathrm{f}}^{0}=\frac{K_2^{0}}{K_3^{0}}=\frac{K_2}{K_3}; \tag{1} \]

\[ \gamma_{\mathrm{p}}^{0}=\frac{500zD_1^{0.45}}{K_3^{0}}; \tag{2} \]

\[ \gamma_{\mathrm{k}}^{0}=100,\quad (3);\qquad \gamma_{0}^{0}=\frac{\gamma_{\mathrm{f}}^{0}}{\gamma_{\mathrm{p}}^{0}},\quad (4);\qquad \gamma_{\mathrm{e}}^{0}=100\gamma_{0}^{0},\quad (5);\qquad \gamma_{\mathrm{ch}}^{0}=100\gamma_{\mathrm{f}}^{0},\quad (6). \]

\[ K_3^{0}=K_3\frac{0.1}{w^{1/2}},\quad (7);\qquad K_3=\frac{I_3}{SC},\quad (8);\qquad K_2=\frac{zFr}{3}\frac{I_2}{q},\quad (9). \]

\(K_1, K_2, K_2^{0}, K_3, K_3^{0}\)—constants of electrolysis of the anodic wave and cathodic peak (the superscript \((^{0})\) denotes standard conditions);
\(w\)—rate of change of potential, V/sec;
\(I_2, I_3\)—anodic and cathodic currents, A;
\(S\)—area of the mercury dropping electrode, cm\(^2\);
\(C_1\)—concentration of ions in solution, mole/ml;
\(F\)—Faraday number (96500);
\(r\)—radius of the mercury dropping electrode, cm;
\(z\)—number of electrons;
\(q\)—area under the anodic wave, coulombs.

Up to the present time, the literature contains no information on the determination of the polarographic coefficients of elements. The availability of these data would make it possible to draw conclusions about the comparative sensitivity, reversibility of electrode processes, etc., on different supporting electrolytes.

The present work is devoted to determining the polarographic coefficients of elements most reliably determined by the method

Table

Polarographic coefficients obtained for various elements
in several supporting electrolytes

Supporting electrolyte Element $K_2^0$ $K_3^0$ $\gamma_{\mathrm{n}}^0$ $\gamma_{\phi}^0$ $\gamma_0^0$ $\gamma_{\mathrm{e}}^0$ $\gamma_{\mathrm{ch}}^0$ $D_1 \cdot 10^5$, cm$^2$ sec$^{-1}$
0.25 M HCl Cu 290 46 0.067 6.8 102 10200 680 0.26
0.25 M HCl Pb 255 50 0.169 5.1 31.0 3100 510 0.824
0.25 M HCl Tl 92.5 16.5 0.205 5.7 27.8 27800 570 1.5
0.1 M NaF Cu 250 80 0.05 3.2 64.0 6400 320 0.404
0.1 M NaF Pb 192.5 60 0.087 3.2 36.0 3600 320 0.855
0.1 M NaF Cd 130 61.5 0.072 3.1 43.0 4300 310 0.597
0.1 M NaF Tl 70.5 22 0.172 3.2 18.6 1860 320 1.88
0.1 M NaF Zn 207 60.5 0.083 3.3 39.8 3980 330 0.76
0.1 M KCl Cu 127 50 0.05 2.25 45.0 4500 225 0.184
0.1 M KCl Pb 220 60 0.089 3.2 36.0 3600 320 0.824
0.1 M KCl Tl 120 24 0.148 5 33.8 3380 500 1.74
0.1 M KCl Cd 215 87.7 0.055 3.5 63.5 6350 350 0.67
0.1 M NH$_4$OH + 0.1 M NH$_4$Cl Cu 123 50 0.105 2.5 23.7 2370 250 0.85
0.1 M NH$_4$OH + 0.1 M NH$_4$Cl Pb 250 60 0.08 4.1 51.0 5100 410 0.675
0.1 M NH$_4$OH + 0.1 M NH$_4$Cl Cd 215 57.7 0.0675 3.5 52.0 5200 350 0.427
0.1 M NH$_4$OH + 0.1 M NH$_4$Cl Zn 117 54 0.16 2.1 13.1 1310 210 2.6
0.1 M NH$_4$OH + 0.1 M NH$_4$Cl Tl 75 26 0.077 3 3.9 3900 300 0.46
0.1 M CH$_3$COONa Cu 180 88 0.0477 2 42.3 4230 205 0.515
0.1 M CH$_3$COONa Pb 167 70 0.078 2.4 30.5 3050 240 0.925
0.1 M CH$_3$COONa Cd 160 44 0.104 3.5 33.6 3360 350 0.64
0.1 M CH$_3$COONa Zn 120 75 0.06 1.6 26.6 2660 160 0.601
0.1 M CH$_3$COONa + 0.1 M CH$_3$COOH Cu 180 80 0.056 2.2 39.2 3920 225 0.57
0.1 M CH$_3$COONa + 0.1 M CH$_3$COOH Pb 197 60 0.0895 3.28 36.6 3660 328 0.91
0.1 M CH$_3$COONa + 0.1 M CH$_3$COOH Cd 190 48 0.093 6 64.5 6450 600 0.622
0.1 M NH$_4$OH + 0.1 M (NH$_4$)$_2$C$_2$H$_4$O$_6$ Cu 82 56.7 0.089 1.45 16.3 1630 145 0.78
0.1 M NH$_4$OH + 0.1 M (NH$_4$)$_2$C$_2$H$_4$O$_6$ Pb 101.6 56.7 0.064 1.79 28.0 2800 179 0.4
0.1 M NH$_4$OH + 0.1 M (NH$_4$)$_2$C$_2$H$_4$O$_6$ Cd 134 121 0.089 1.11 28.5 2850 111 0.7
0.1 M NH$_4$OH + 0.1 M (NH$_4$)$_2$C$_2$H$_4$O$_6$ Zn 118 158 0.035 0.747 21.3 2130 74.7 0.97
0.1 M NH$_4$OH + 0.1 M (NH$_4$)$_2$C$_2$H$_4$O$_6$ Tl 38 91.3 0.089 0.416 10.7 1070 4.16 1.8

Continuation of the table

1 2 3 4 5 6 7 8 9 10
0.1 M NH₄OH + 0.3 M (NH₄)₂C₄H₄O₆ Cu 82 58,2 0,077 1,41 18,3 1830 141 0,62
0.1 M NH₄OH + 0.3 M (NH₄)₂C₄H₄O₆ Pb 103 47 0,079 2,19 27,6 2760 219 0,4
0.1 M NH₄OH + 0.3 M (NH₄)₂C₄H₄O₆ Cd 164,5 120 0,040 1,37 34,2 3420 137 0,7
0.1 M NH₄OH + 0.3 M (NH₄)₂C₄H₄O₆ Zn 121,2 158 0,0356 0,766 21,5 2150 76,6 0,97
0.1 M NH₄OH + 0.3 M (NH₄)₂C₄H₄O₆ Tl 41 80,3 0,045 0,51 11,3 1130 51 1,8
0.1 M NH₄OH + 0.6 M (NH₄)₂C₄H₄O₆ Cu 70 59,7 0,077 1,17 15,2 1520 117 0,54
0.1 M NH₄OH + 0.6 M (NH₄)₂C₄H₄O₆ Pb 108,5 48 0,077 2,26 29,4 2940 226 0,4
0.1 M NH₄OH + 0.6 M (NH₄)₂C₄H₄O₆ Cd 122 108 0,0445 1,13 25,4 2540 113 0,7
0.1 M NH₄OH + 0.6 M (NH₄)₂C₄H₄O₆ Zn 230 157 0,035 1,46 41,6 4160 146,4 0,97
0.1 M NH₄OH + 0.6 M (NH₄)₂C₄H₄O₆ Tl 38,8 82 0,0441 0,47 10,6 1060 47 1,8
0.3 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Cu 79 67,6 0,063 1,17 18,6 1860 117 0,54
0.3 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Pb 98,4 57,5 0,065 1,71 26,3 2630 171 0,4
0.3 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Cd 141 131 0,0365 1,08 29,5 2950 108 0,7
0.3 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Zn 117 165 0,034 0,71 21,0 2100 71 0,97
0.3 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Tl 36,8 86,5 0,042 0,426 10,2 1020 42,6 1,8
0.6 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Cu 77,5 67,6 0,068 1,14 16,8 1680 114 0,54
0.6 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Pb 112 58 0,064 1,93 30,0 3000 193 0,4
0.6 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Cd 131 138 0,035 0,95 27,0 2700 95 0,7
0.6 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Zn 113 172 0,0327 0,66 29,0 2900 66 0,97
0.6 M NH₄OH + 0.1 M (NH₄)₂C₄H₄O₆ Tl 40 82 0,044 0,488 11,1 1110 48,8 1,8

amalgam polarography with accumulation (Cu, Pb, Sb, Cd, Zn; Tl, Bi, Sn, Ga), in several electrolytes frequently used in polarographic analysis (0.1 M NaF; 0.1 M NH\(_4\)OH + 0.1 N NH\(_4\)Cl; 0.1 M KCl; 0.1 M CH\(_3\)COONa; 0.25 M HCl; 0.1 M CH\(_3\)COONa + 0.1 M CH\(_3\)COOH; \(m\)M NH\(_4\)OH + \(n\)M (NH\(_4\))\(_2\)C\(_4\)H\(_4\)O\(_6\)). It should be noted that, for some of the indicated elements in the electrolytes studied, anodic waves were not obtained.

The table gives the mean values of the experimental data obtained from three measurements. It is evident from the table that the sensitivity coefficients (\(\gamma_{\mathrm{ч}}^{0}\)) of different elements, and of the same element in different supporting media, may differ. Fluctuations in the values of the sensitivity coefficients of one element in different supporting media, at the same concentration coefficient, are due to the degree of reversibility of the electrode process. For example, for Zn, for which among all the divalent elements studied the electrode process in the medium 0.1 M NH\(_4\)Cl + 0.1 M NH\(_4\)OH is the most irreversible, the value of \(\gamma_{\mathrm{ч}}^{0}\) is the smallest. The magnitude \(\gamma_{\mathrm{ч}}^{0}\) also depends on the diffusion coefficients of metal atoms in mercury.

The electrolysis coefficients (\(\gamma_{\mathrm{э}}^{0}\)) and other coefficients of different elements differ considerably from one another, which is also due to the different degree of reversibility of the electrode processes.

From a comparison of the sensitivity coefficients for zinc in several supporting media, it is evident that the sensitivity of zinc determination in 0.1 M NaF is approximately twice as high as that in 0.1 M CH\(_3\)COONa. To achieve the same degree of concentration (\(\gamma_{\mathrm{k}}^{0}=100\)) when carrying out electrolysis in the media 0.1 M NaF and 0.1 M NH\(_4\)OH + 0.1 M NH\(_4\)Cl, in the second medium the intensity of stirring of the solution must be approximately 1.9 times greater than in the first medium. From a comparison of \(\gamma_{0}^{0}\) in the first and second media, it is seen that the ratio between the constants of the anodic current and the electrolysis current in the first medium is more favorable than in the second. A comparison of \(\gamma_{\mathrm{э}}^{0}\) for zinc in different supporting media shows that in 0.1 M NaF the current of anodic dissolution of zinc amalgam exceeds the electrolysis current to a considerably greater extent than in 0.1 M NH\(_4\)OH + 0.1 M NH\(_4\)Cl and 0.1 M CH\(_3\)COONa, which also accounts for the larger value of \(K_{2}^{0}\) in the first medium compared with the other two media.

From the values of \(\gamma_{\phi}^{0}\) for zinc in the indicated supporting media, it is evident that in 0.1 M NaF the anodic peak, in comparison with the cathodic one, is sharper than in the other two media. Analogous comparisons can also be made for other elements. Thus, the experimental data obtained show that, in accordance with theoretical considerations, the above polarographic coefficients may serve as characteristics of the sensitivity of element determination and of the reversibility of electrode processes.

In conclusion, we express our gratitude to Professor A. G. Stromberg for his attention to the work.

Conclusions

For a number of elements in several supporting media, amalgam-polarographic coefficients have been obtained which characterize the sensitivity of element determination and the degree of reversibility of their electrode processes.

References

  1. M. S. Zakharov, A. G. Stromberg. Journal of Analytical Chemistry, 19, 913, 1964.

  2. A. G. Stromberg, M. S. Zakharov. Journal of Analytical Chemistry (in press).

Submission history

Polarographic Coefficients of Some Elements in the Method of Amalgam Polarography with Accumulation