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Chemical Thermodynamics of Tin - Volume 12 - OECD Nuclear ...

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428<br />

A Discussion <strong>of</strong> selected references<br />

4−x<br />

Table A-77: Formation constants β x <strong>of</strong> SnClx<br />

complexes (units on the molality basis)<br />

determined in HClO 4 background solutions at different ionic strength (the estimated<br />

experimental errors (3σ) are in parentheses) and extrapolated values to zero ionic<br />

strength and to I m = 6.41 mol kg –1 by SIT.<br />

I m (I c ) log 10 β 1 log 10 β 2 log 10 β 4 log 10 β 5 log 10 β 6<br />

5.62 (4.5) 2.91(0.36) 4.96(0.36) 8.01(0.30) 8.91(0.45) 8.40(0.50)<br />

7.42 (5.6) 2.80(0.30) 5.19(0.30) 8.75(0.30) 9.81(0.40) 9.89(0.40)<br />

8.<strong>12</strong> (6.0) 3.13(0.<strong>12</strong>) 5.77(0.10) 9.27(0.<strong>12</strong>) 10.20(0.15) 10.15(0.18)<br />

10.03 (7.0) 3.52(0.15) 6.57(0.<strong>12</strong>) 10.39(0.10) 11.38(0.10) 11.69(0.<strong>12</strong>)<br />

<strong>12</strong>.18 (8.0) 4.40(0.30) 7.45(0.15) 11.69(0.10) <strong>12</strong>.43(0.<strong>12</strong>) <strong>12</strong>.67(0.15)<br />

→ 0 † 3.19 ± 0.50 5.95 ± 0.36 9.57 ± 0.32 10.93 ± 0.41 9.83 ± 0.49<br />

Δε/kg·mol –1 – 0.26 ± 0.06 – 0.45 ± 0.04 – 0.64 ± 0.03 – 0.60 ± 0.04 – 0.67 ± 0.05<br />

→ 6.41 ‡ ← 2.73 ± 0.17 5.08 ± 0.14 8.31 ± 0.14 9.38 ± 0.17 9.28 ± 0.20<br />

†<br />

‡<br />

Extrapolation to zero ionic strength by weighted linear regression and error propagation assuming<br />

Gaussian probability distribution, and 95% confidence limits <strong>of</strong> parameters [2003BEV/ROB].<br />

Interpolation to average ionic strength I m = 6.41 mol·kg –1 .<br />

For the right side, a Hg-pool electrode has been constructed, which is<br />

connected to the outside environment via a Pt-wire welded into the bottom <strong>of</strong> the glass<br />

wall <strong>of</strong> the compartment. This compartment also has a tightly fitted Teflon lid, with<br />

three inlets: in one, high purity (99.996%) Ar purging gas is led to the system, the other<br />

one for admitting the titrant solutions in the cell and the third one for venting. The<br />

quality <strong>of</strong> Ar was checked with bubbling the gas through alkaline pyrogallol solution;<br />

extensive bubbling, for a couple <strong>of</strong> hours, did not cause any discoloration in the<br />

solution, which proves, that O 2 content <strong>of</strong> the Ar-gas can be considered as insignificant.<br />

The lack <strong>of</strong> O 2 was also checked via adding I – ions to the background solutions;<br />

resulting in no visually detectable I 2 formation (in strongly acidic solutions O 2 readily<br />

oxidises I – ion). This control reaction also proved, that other oxidants (i.e., traces <strong>of</strong><br />

ClO − , Cl 2 ) are absent from HClO 4 and HClO 4 -HCl background electrolytes as well.<br />

3<br />

Platinised Pt-electrodes were prepared according to the literature<br />

[1998SIP/HEF]. The electrode consists <strong>of</strong> high purity (99.999%) Pt-wire (d = 1.5 mm)<br />

and 5 mm × 8 mm high purity (99.999%) Pt-sheets. The platinisation was performed<br />

(after careful cleaning, as described in [1934BRO], by using H 2 PtCl 6 in strongly acidic<br />

HCl ([HCl] TOT = 0.2 M) solution. The two electrodes were connected to a high<br />

impedance multimeter via crocodile clips.<br />

The experimentally observed potential values as a function <strong>of</strong><br />

o<br />

lg([Sn(IV) free ]/[Sn(II) free ]) are depicted in Figure A-51. The evaluation <strong>of</strong> E (Sn 4+ /Sn 2+ )<br />

in chloride containing media requires the knowledge <strong>of</strong> the stepwise formation<br />

2−x<br />

4 x<br />

constants <strong>of</strong> the complexes SnClx<br />

and SnCl<br />

−<br />

x<br />

. For the former the values selected in<br />

this review were used, and the pertinent values for the latter are listed in Table A-78.<br />

CHEMICAL THERMODYNAMICS OF TIN, ISBN 978-92-64-99206-1, © <strong>OECD</strong> 20<strong>12</strong>

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