ORNL-1816 - the Molten Salt Energy Technologies Web Site
ORNL-1816 - the Molten Salt Energy Technologies Web Site
ORNL-1816 - the Molten Salt Energy Technologies Web Site
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ANP QUARTERLY PROGRESS REPORT<br />
TABLE 5.8. PHASES FOUND IN MF-UF3 BINARY MIXTURES<br />
Lattice<br />
Molar Compositiona Phases Structure Type<br />
Zb<br />
Dimensions (A)<br />
2NaF-lUF3 Hexagonal phase ond p2- N aU F4 a = 6.17<br />
3NaF-2U F3 also NaF c = 3.78<br />
1KF-1UF3 Hexagonal phase and P,-KUF4 a = 6.51<br />
cubic phaseC c = 3.76<br />
F I uorite type a. = 5.9<br />
1 K F - 1 Na F-2U F3 Two hexagonal phases @2%Na)UF4 a = 6.27<br />
c = 7.71<br />
3<br />
3<br />
4<br />
3<br />
4<br />
P,-KUF4 a = 6.51 %<br />
c = 3.76<br />
aSomples prepored by V. S. Coleman and W. C. Whitley and examined petrographically by T. N. McVay.<br />
bThe number of molecules per unit cell.<br />
CThis phase may be <strong>the</strong> cubic phase of KUF4 or <strong>the</strong> compound UOF with <strong>the</strong> fluorite structure.<br />
and So = 29.90 e.u., of which 0.53 e.u. was obtained<br />
by extrapolation below 20°K.<br />
The heat capacity of a sample of pure MoS,<br />
was measured from about 15OK to room temperature.<br />
The heat capacity and <strong>the</strong> derived <strong>the</strong>rmodynamic<br />
functions mentioned above were tabulated at 10-deg<br />
intervals up to 300OK. At 298.15'K, C, = 15.62<br />
cal/mole*°K, and So = 15.34 e.u. The heat capacity<br />
of MoS, follows a T2 dependence between<br />
15 and about 70°K of <strong>the</strong> sort previously reported3'<br />
for MOO,. This behavior of MoS, is consistent<br />
with its layer structure, which is so pronounced<br />
that MoS, actually is a good high-temperature<br />
I ubri cant (L iqu i-Mol y).<br />
Density and electrical conductance measurements<br />
were made of molten mixtures of KCI and KI across<br />
<strong>the</strong> entire composition face. The molar volume, as<br />
calculated from <strong>the</strong> density, is nearly additive<br />
for this system, although it shows deviations close<br />
to <strong>the</strong> KI side. In contrast, <strong>the</strong> equivalent conuctance<br />
shows pronounced negative deviations<br />
additivity for all mixtures, with maximum<br />
ation at high KCI concentration. These data<br />
in show that it is inadvisable to interpret<br />
maximums and minimums in electrical conductance<br />
as <strong>the</strong> consequence of formation of compounds in<br />
34E. R. Van Artsdalen, ANP Quay. Prog. Rep. Sept.<br />
10, 1954, <strong>ORNL</strong>-1771, p 72.<br />
* r<br />
*<br />
<strong>the</strong> melts. The specific conductivity of molten -<br />
KI is expressed by <strong>the</strong> equation r "<br />
K = -1.7100 + 6,408 x 10-3t<br />
- 2.965 x 10-6t2 mho/cm<br />
between 725 and 925OC, and <strong>the</strong> density is given<br />
by <strong>the</strong> equation<br />
p = 3.0985 - 0.9557 x 10-3t g/sm3<br />
between 680 and 91OOC. The temperature, t, is<br />
in OC.<br />
The density and electrical conductance were<br />
determined for pure molten NaBr and are given<br />
below for <strong>the</strong> range 750 to 960OC:<br />
K = -0.4392 + 5.632 x 1013t<br />
- 1.572 x 10-6t2 mho/cm<br />
and<br />
p = 2.9518 - 0.8169 x 10-3t g/cm3.<br />
The self-diffusion coefficient of sodium ion in<br />
molten NaNO, has been determined by a radiochemical<br />
tracer technique. The heat of activation<br />
for self-diffusion is approximately 6 kcal/mole and,<br />
-<br />
<strong>the</strong>refore, higher than <strong>the</strong> heat of activation for<br />
electrical conductance. Similar work with thallous<br />
chloride35 has shown that <strong>the</strong> heat of activation<br />
7 ,<br />
.<br />
35E. Berne and A. Klernm, Z. Naturforsch. 8a, 400<br />
(1953).<br />
c<br />
-