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ORNL-2106 - the Molten Salt Energy Technologies Web Site

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UNIF, = yN should be unity (a pure solid has unit<br />

activity). The apparent activity is 9 at 600°C and<br />

20 at 70O0C, however, which indicates that <strong>the</strong><br />

saturating phase is something less soluble than<br />

NiF,. The discrepancy amounts to a factor of<br />

10 in <strong>the</strong> activity coefficient or <strong>the</strong> solubility and<br />

to about 5 kcal/mole in <strong>the</strong> value of AFF;,F2. In<br />

computing <strong>the</strong> AF" for <strong>the</strong> formation of <strong>the</strong> complex<br />

compound from <strong>the</strong> elements, <strong>the</strong> free energy esti-<br />

mates given in Table 2.2.13 were employed.20<br />

,OL. Brewer et aL, p 104-115 in The Chemistry and<br />

Metallur o Mkcehneous Materials, Thermod namics.<br />

NNES Ivlds, ed. by L. L. Quill, McGraw-dll, New<br />

York, 1950.<br />

TABLE 2.2.13. SELECTED VALUES OF<br />

FREE ENERGY OF FORMATION<br />

bo (kcal/mole)<br />

At 600°C At 700°C<br />

Fe F2 -137.5 -133.9<br />

Cr F2 -1525 -1 48.9<br />

Ni F2 -127.9 -1248<br />

Zr F4 -383.4 -376.8<br />

PERlOD ENOlNC JUNE IO, 1956<br />

An independent check on <strong>the</strong> differences in <strong>the</strong><br />

standardfree energies of formation of <strong>the</strong> MF,*ZrF4<br />

complex from <strong>the</strong> elements is afforded by previously<br />

published data obtained for bimetallic couples in<br />

saturated half To a first approximation,<br />

<strong>the</strong> cel'l reaction was<br />

M + M'F2*ZrF4 = MF2*LrF4 + M' .<br />

This reaction neglects transport and junction poten-<br />

tials, which are small if <strong>the</strong> saturated solutions<br />

are sufficiently dilute. From <strong>the</strong> relation<br />

En3 = -AF<br />

far <strong>the</strong> cell reaction, where E is <strong>the</strong> electromotive<br />

force, R is <strong>the</strong> number of equivalents transferred,<br />

and 3 is <strong>the</strong> number of Faradays passed, an approx-<br />

mate value of <strong>the</strong> difference in <strong>the</strong> free energy of<br />

formation from <strong>the</strong> elements is found. The com-<br />

parison is shown in Table 2.2.14.<br />

The values of AFcalc in Table 2.2.14 were ob-<br />

tained by subtracting <strong>the</strong> values of AFo given for<br />

<strong>the</strong>se complexes in <strong>the</strong> last column of Table 2.2.12.<br />

While <strong>the</strong> agreement is good, <strong>the</strong> effect of <strong>the</strong> high<br />

solubility of GF, at 700°C is probably responsible<br />

for <strong>the</strong> larger of <strong>the</strong> discrepancies.<br />

,'L. E. Topol, ANP Quat. frog. Rep. Sept. 10, 1955,<br />

<strong>ORNL</strong>-1947, p 85.<br />

TABLE 2.2.14. COMPARISON OF FREE ENERGIES OF FORMATION OF MF2*ZrF4<br />

OBTAINED BY TWO METHODS<br />

FeF2*ZrF4-GF2*ZrF4<br />

Difference Between bM F2,fr F4 and &M'F2*ZrF4<br />

(kea Vmo le)<br />

At 600°C At 70OoC<br />

-En 3 . 15.5 16.8<br />

AFcalc 15 15<br />

Fe F2*Zr F4-N i F2* Zr F4<br />

-En 3 -19.5 -20.0<br />

~colc<br />

GFZ*ZrF4-NiF2*ZrF4<br />

-20 -20<br />

-En 3 35.1 -36.3<br />

3 5 3 5<br />

107

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