ORNL-1771 - Oak Ridge National Laboratory
ORNL-1771 - Oak Ridge National Laboratory
ORNL-1771 - Oak Ridge National Laboratory
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UNCLASSIFIED<br />
<strong>ORNL</strong>-LR-OWG 3034<br />
.<br />
I<br />
... .... i<br />
300 500 700 900 1100 !300<br />
TEMPERATURE (OK)<br />
Fig. 6.24. Free Energy Differences as Functions<br />
of Temperature,<br />
There are no satisfactory heat of formation<br />
data for any of the alkali-metal hydroxides other<br />
than those for sodium. Therefore, only the rela-<br />
tive importance of the decomposition equilibria<br />
can be studied. Some of the entropy values for<br />
the higher oxides have been estimated and are<br />
reported in the literature. However, the heats<br />
of formation for rubidium and cesium oxides<br />
are quite uncertain, and it is presently believed<br />
that the accuracy of the AFYIZ and AF';,, values<br />
given in Table 6.12 would not be improved by<br />
use of these entropy estimates. Therefore, only<br />
enthalpy values will be used, but it will be shown<br />
that this restriction is not so serious as it might<br />
at first seem to be.<br />
Comparing equilibria 1 and 2 shows<br />
PERIOD ENDfNG SEPTEMBER lo, 1954<br />
The degree of approximation can be checked by<br />
using the data for sodium compounds. In this case<br />
AFT,2 is -35.5 kcal, when using the approximation,<br />
as compared with the correct value of -40.7 kcal.<br />
Likewise, is -94.2 kcal compared with the<br />
correct value of -94.9 kcal. The approximate<br />
values of and AF;,3 at 25°C are tabulated<br />
in Table 6.12 for all the alkali-metal hydroxides.<br />
Table 6.12 shows that hydrogen and the peroxide<br />
should be produced most readily in potassium hy-<br />
droxide and least readily in lithium hydroxide.<br />
Nevertheless, equilibrium 1 is predominant, and<br />
equilibrium 3 and hence equilibrium 4 are insigni-<br />
ficant.<br />
TABLE 4.12. APPROXIMATE<br />
AND AF;,3 AT 25OC<br />
M A";, 2<br />
(kcal)<br />
Li -47<br />
No -36<br />
K -25<br />
Rb -34<br />
cs -35<br />
Aq, 3<br />
(kcal)<br />
- 94<br />
-76<br />
- 73<br />
- 70<br />
Various investigations of corrosion and mass<br />
transfer hove shown the fundamental role played<br />
by hydrogen. The above computations show that<br />
hydrogen is important in stabilizing sodium hy-<br />
droxide at temperatures above 6QO"C, as shown in<br />
All the data required in the above equation are<br />
-__available,<br />
except those for the entropy term. Since Table 6.11. This is the temperature range at which<br />
this term represents a difference in entropy for two mass transfer becomes significant. These compu-<br />
similar substances, it may be supposed that its tations also link the formation of hydrogen with<br />
omission will not be serious. A similar situation the formation of unsaturated oxygen ions. As will<br />
obtains for AFY,3. Hence, the following approxi- be shown in a subsequent report, the presence of<br />
motions will be used.<br />
these unsaturated ions may be necessary for mass<br />
107