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ORNL-1771 - Oak Ridge National Laboratory

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ANP QUARTERLY PROGRESS REPORT<br />

The existence of these equilibria is coinpatible shown in ?able 6.11 were obtained. The pressure-<br />

with Eq. ha, as may be seen from the fact that activity coefficient products in this table give the<br />

AFY = AF; - AF;, K,,, = K ~ / K ~ Hence . it pressures which would be obtained if the solutions<br />

woucd have been possible to derive Eq. Sa by using were ideal. Figure 1.23 shows the relative im-<br />

equilibria 7 and 3. This is because the two sets portance of equilibria 1 and 2 in terms of the loga-<br />

of equilibria 1 and 2 and equilibria 7 and 8 are<br />

both equivalent to the one equilibrium<br />

From Eq. 9 it will be noted that the pressure ratio<br />

(Pt+20'PH2 )1,2<br />

is determined by the competition<br />

between the oxide and hydrogen for oxygen, with<br />

the one trying to form the peroxide and the other<br />

trying to form water.<br />

In like manner, an expression analogous to Eq.<br />

6a can be derived under the assumption that equi-<br />

libria 1 and 3 determine the water and hydrogen<br />

pressures, respectively. This expression is<br />

K1,3 =--- ,<br />

K3'l3<br />

rithm of the pressure ratio as a function of the<br />

reciprocal of the absolute temperature. Figure<br />

6.21 gives the free energy differences (AF" and<br />

1,2<br />

AF" ) as functions of absolute temperature.<br />

1,3<br />

Examination of these data shows the following:<br />

(1) Apart From unexpectedly large deviations from<br />

ideality, equilibrium 1 will predominate at all<br />

temperatures. (2) Assuming ideality, hydrogen<br />

evolution from fused sodium hydroxide in an inert<br />

container will be small at all temperatures, but it<br />

should be measurable at 906°C. Likewise, the<br />

peroxide concentration at al I temperatures may be<br />

small, but it should be appreciable at 900°C. (3)<br />

Deviations from ideality of a moderate amount<br />

could make hydrogen and peroxide formation either<br />

insignificant or greatly important at high temper-<br />

atures.<br />

62<br />

54<br />

46<br />

38<br />

r<br />

~~<br />

UNCLASSIFIED<br />

ORPll -l-R-DNG 3033<br />

30L - -<br />

60 80 10 0 420 14 0 160<br />

(!/TEMPERATURE) x io4 (OK)-'<br />

By using the free energy data computed above Fig. 6.23. Decomposition Pressure Functions<br />

for sodium hydroxide, the representative values for NaQaH.<br />

1 06<br />

Temperature AFY At.;<br />

TABLE 6.11. DATA ON THE DECOMPQSlTlON OF SODIUM HYDROXIDE<br />

("a (kcal) (kcal) K1 K2 K3<br />

~.~~~...~~ _. ..~.<br />

~~ ~<br />

25 35.3 76.0 10 -26 10-56 10-95<br />

600 21.4 64.4 4.7 x 10-6 10-18 10-27<br />

(mm Hg)<br />

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

(mm Hg)<br />

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

1.7 7.4 x 10-6<br />

900 13.5 59.9 3 x 1 ~ - 3 8 x lC-18 42.0 2.1

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