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

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VII.2 Solid tin oxides and hydroxides 119<br />

Hirayama [1964HIR] stated that the entropy <strong>of</strong> this compound is reported<br />

(source unknown) to be (56.5 ± 1.3) J·K –1·mol –1 ο<br />

. If we use the value <strong>of</strong> (Sn, cr,<br />

white, 298.15 K) = (51.18 ± 0.08) J·mol –1·K S m<br />

–1 selected in this review, and the CODATA<br />

value for oxygen as (205.152 ± 0.005) J·K –1·mol –1 , the calculated entropy <strong>of</strong> formation<br />

is − 97.26 J·mol –1·K –1 ο<br />

and the resulting Δ is − 257.00 kJ·mol –1 fGm<br />

. Humphrey and<br />

O’Brien’s value for the enthalpy <strong>of</strong> formation (− 286.00 kJ·mol –1 ) differs considerably<br />

from the value measured by Lavut et al. [1981LAV/TIM] who determined the enthalpy<br />

ο<br />

<strong>of</strong> formation <strong>of</strong> SnO(cr) as: Δ fHm(SnO, tetragonal, 298.15 K) = − (280.71 ± 0.21)<br />

kJ·mol –1 . They used a well characterised sample in combustion calorimetry, the same<br />

method as used in [1953HUM/OBR]. The enthalpy <strong>of</strong> SnO(cr) differs from that<br />

reported in [1953HUM/OBR] significantly by almost 2%. The large discrepancy<br />

between the combustion calorimetric results cannot be resolved by looking at only these<br />

two sets <strong>of</strong> data. Arguments favouring the data by Lavut et al. [1981LAV/TIM] are<br />

based on a) high purity tin specimens, b) a reliable method <strong>of</strong> determining the reaction<br />

completeness, and c) a higher degree <strong>of</strong> combustion <strong>of</strong> tin. Lavut et al. also question the<br />

presence <strong>of</strong> water in gas form in the bomb which was not accounted for by Humphrey<br />

and O’Brien.<br />

A quite thorough review <strong>of</strong> the available data ([1978COX], [1979GLU/MED],<br />

[1982WAG/EVA], [1982PAN]) was provided by Lamoreaux and Hildenbrand<br />

ο<br />

[1987LAM/HIL]. Their recommended values for Δ fHm(SnO, cr, 298.15 K) and<br />

ο<br />

S (SnO, cr, 298.15 K) are − (280.681 ± 0.166) kJ·mol –1 m<br />

and (57.167 ± 0.291)<br />

J·K –1·mol –1 respectively. The value <strong>of</strong> the enthalpy <strong>of</strong> formation <strong>of</strong> SnO(cr) is found to<br />

be consistent with the evaluation by [1979GLU/MED], [1978COX] and [1982PAN] but<br />

different from [1982WAG/EVA]. The entropy value is as in [1979GLU/MED] but<br />

different from others.<br />

Solov’ev et al. [2001SOL/VLA] measured the enthalpies <strong>of</strong> reactions <strong>of</strong><br />

SnO(cr) and SnF 2 (cr) with hydr<strong>of</strong>luoric acid in an isothermic-shell calorimeter. They<br />

used the reaction:<br />

SnO(cr) + 3 HF(l) H[SnF 3 ](l) +H 2 O(l)<br />

and obtained a value <strong>of</strong> − (67.2 ± 1.4) kJ·mol –1 for the enthalpy <strong>of</strong> reaction but did not<br />

ο<br />

complete the thermochemical cycle to get the data for Δ H (SnO, cr, 298.15 K).<br />

The data <strong>of</strong> [1981LAV/TIM] and two critical reviews [1987LAM/HIL] and<br />

[1991GUR/VEY] support the higher value <strong>of</strong> enthalpy, while the dataset <strong>of</strong> Humphrey<br />

and O'Brien [1953HUM/OBR] using the same calorimetric method favours the lower<br />

value. There are two other determinations <strong>of</strong> enthalpy, one by Maier [1929MAI] who<br />

measured the potentials <strong>of</strong> galvanic cells and obtained − (285.4 ± 4.0) kJ·mol –1 and the<br />

second by Garrett and Heiks [1941GAR/HEI] who used solubility measurements and<br />

obtained − (283.9 ± 3.0) kJ·mol –1 . It will be shown in Section VII.2.2.4 that the data <strong>of</strong><br />

ο<br />

[1981LAV/TIM] cannot be taken into account for the evaluation <strong>of</strong> ΔfH m(SnO, cr,<br />

298.15 K).<br />

f<br />

m<br />

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

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