ORNL-2106 - the Molten Salt Energy Technologies Web Site
ORNL-2106 - the Molten Salt Energy Technologies Web Site
ORNL-2106 - the Molten Salt Energy Technologies Web Site
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ANP PROJECT PROGRESS REPORT<br />
The recent system modification resulted in a<br />
temperature rise of 33OF for <strong>the</strong> sodium coolant<br />
stream and a maximum boron carbide temperature<br />
of 1526OF for a sodium inlet temperature of 12OOOF.<br />
These values may be compared with <strong>the</strong> previous<br />
results for a system without <strong>the</strong> copper-boron<br />
carbide matrix in which <strong>the</strong> sodium temperature<br />
rise was 24OF and <strong>the</strong> boron carbide attained a<br />
maximum temperature of 1586OF. The sodium<br />
temperature rise was found to vary 10% (decreasing<br />
from 36 to 33OF) when <strong>the</strong> sodium inlet temper-<br />
ature was changed from 1150 to 1200OF. Typical<br />
temperature profiles at <strong>the</strong> inlet and outlet ends<br />
of <strong>the</strong> system for a sodium inlet temperature of<br />
1175’F are presented ih Fig. 4.1.15, and <strong>the</strong><br />
temperature profiles for <strong>the</strong> system without <strong>the</strong><br />
Cu-B,C (System 8) are also shown for comparison.<br />
13C. J. Barton, Fused <strong>Salt</strong> Compositions, <strong>ORNL</strong><br />
CF-55-9-78 (Sew. 16, 1955).<br />
230<br />
NaF-LiF-ZrF,(22-55-23 mole %)<br />
Beta form (106 to 3680C)<br />
HT - H30°C<br />
c<br />
P<br />
Alpha form (407 to 556OC)<br />
The system modification increased <strong>the</strong> temper-<br />
ature drop across <strong>the</strong> inner lnconel shell by 30 to<br />
35°F. The temperature gradient in <strong>the</strong> outer<br />
lnconel shell was essentially unchanged.<br />
HEAT CAPACITY<br />
W. D. Powers<br />
The enthalpies and heat capacities of two<br />
mixtures were determined in <strong>the</strong> liquid and solid<br />
states. For one mixture, NaF-LiF-ZrF, (22-55-23<br />
mole %), two distinct discontinuities in <strong>the</strong> temper-<br />
ature-enthalpy relationship were found; one was at<br />
370 to 380°C and <strong>the</strong> o<strong>the</strong>r was at 565 to 585°C.<br />
The reported13 fiquidus temperature is 57OoC.<br />
The lower discontinuity is assumed to be a phase<br />
transition from <strong>the</strong> alpha form to <strong>the</strong> beta form, <strong>the</strong><br />
beta form being stable below 375OC. The dis-<br />
continuity at <strong>the</strong> higher temperature is <strong>the</strong> fusion<br />
of <strong>the</strong> alpha form to <strong>the</strong> liquid at 570°C. Enthalpy<br />
and heat capacity measurements of a second salt<br />
mixture, LiF-NoF (60-40 mole %), showed no<br />
unusual characteristics. The enthalpy and heat<br />
capacity equations for <strong>the</strong>se two salts follow:<br />
= -8.7 + 0.2392T + (7.20 x 10-’)T2<br />
= 0.2392 + (14.39 x lO-’)T<br />
HT - H30°C = 64.2 - 0.009165T + (41.82 x 10m5)T2<br />
c = -0.009165 + (83.64 x lO”)T<br />
P<br />
Liquid (603 to 897°C)<br />
HT - H3,,oC = -20.2 + 0.4526T - (5.95 x 10-’)T2<br />
At 375OC<br />
At 57OOC<br />
c = 0.4526 - (11.89 x lO-’)T<br />
P<br />
Ha- Hg = 28<br />
Hliq - Ha = 24<br />
LiFNaF (60-40 mole %)<br />
Solid (1 12 to 572OC)<br />
HT - H30°C<br />
c<br />
P<br />
= -9.8 + 0.3191T + (9.94 x 10”)T2<br />
= 0.3191 - (19.87 x lO”)T<br />
-<br />
W<br />
..-<br />
t<br />
c<br />
.