02.05.2014 Views

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

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

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

202<br />

VIII Group 17 (halogen) compounds and complexes<br />

This selection yields:<br />

Δ G (SnBr 2 , g, 298.15 K) = − (155.8 ± 4.3) kJ·mol –1 .<br />

f<br />

ο<br />

m<br />

From mass spectrometric measurements on the vapour above liquid tin(II)<br />

bromide evidence was found for the existence <strong>of</strong> dimers Sn 2 Br 4 [1969KAR2]. This<br />

finding was corroborated later in more detailed measurements [1991HIL/MIL2],<br />

[1992BRU/WAL2]. Partial pressures <strong>of</strong> monomer and dimer in the vapour phase were<br />

determined by [1991HIL/MIL2] between 423 and 573 K. Their data, when extrapolated<br />

to 298 K, indicate that the mole fraction <strong>of</strong> dimers in the gas phase is approximately<br />

0.01.<br />

VIII.4.3.2 SnBr 4 (g)<br />

Ideal gas properties <strong>of</strong> gaseous SnBr 4 were calculated by [1962ANA] and<br />

[1991GUR/VEY] from spectroscopic and structural data. The data were those <strong>of</strong><br />

[1941LIS/SUT], [1973DER/KOV], [1971CLA/RIP], [1972CLA/RIP],<br />

[1972CLA/RIP2], [1954DEL/FRA], [1977KON/MUL], [1971CLA/WIL],<br />

[1979CRE/SIN], [1976KON/MUL] and [1963MOS]. Gurvich and Veyts<br />

[1991GUR/VEY] re-evaluated the data and performed the caculations using the rigid<br />

rotator-harmonic oscillator approximation. Reported data appear in Table VIII-26.<br />

Table VIII-26: Ideal gas properties <strong>of</strong> SnBr 4 from compilations/evaluations (C/E) and<br />

original article (A).<br />

ο<br />

p,m<br />

S m<br />

ο<br />

Reference<br />

C (SnBr 4 , g, 298.15 K)/ (SnBr 4 , g, 298.15 K)/<br />

ο<br />

Δ fHm<br />

(SnBr 4 , g, 298.15 K)/<br />

–1<br />

J·K<br />

–1·mol<br />

–1<br />

J·K<br />

–1·mol kJ·mol –1<br />

[1962ANA] (A) 103.4 4<strong>12</strong>.6 -<br />

[1991GUR/VEY] (C/E) 103.284 (a) 413.228 (a) − 324.217 ± 4.5 (a)<br />

[1973BAR/KNA] (C/E) 103.34 411.8 − 314.6<br />

[1993BAR] (C/E) 103.422 4<strong>12</strong>.652 − 348.109<br />

[1999BIN/MIL] (C/E) 103.3 4<strong>12</strong>.4 − 347.6<br />

[1982WAG/EVA] (C/E) - - − 314.6<br />

(a) Selected data.<br />

The standard enthalpy <strong>of</strong> formation <strong>of</strong> gaseous SnBr 4 may be derived from data<br />

for the condensed phase compound. In Section VIII.1.3.2, the value<br />

f<br />

ο<br />

m<br />

Δ H (SnBr 4 , cr, 298.15 K) = − (388.0 ± 3.0) kJ·mol –1<br />

was selected. The enthalpy <strong>of</strong> sublimation may be deduced from vapour pressure<br />

measurements. Table VIII-27 summarises vapour pressure data sources. The enthalpy <strong>of</strong><br />

sublimation was derived from these data, with the use <strong>of</strong> evaluated auxiliary data for<br />

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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!