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ORNL-1771 - Oak Ridge National Laboratory

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........<br />

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

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