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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 />

.

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