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ORNL-2106 - the Molten Salt Energy Technologies Web Site

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supporting plaque is loaded into <strong>the</strong> tube through<br />

<strong>the</strong> sample-loading flange. The central portion<br />

of <strong>the</strong> tube is <strong>the</strong>n baked out under high vacuum<br />

to remove volatile materials which might con-<br />

taminate <strong>the</strong> surface of <strong>the</strong> sample. After <strong>the</strong><br />

furnace is adjusted to <strong>the</strong> operating temperature,<br />

<strong>the</strong> sample is pushed to <strong>the</strong> center of <strong>the</strong> constant-<br />

tern perature block with <strong>the</strong> so lenoidspera ted<br />

sample-manipulating rods. Photographs are taken<br />

of <strong>the</strong> sample as a function of time to ensure <strong>the</strong><br />

establishment of an equilibrium droplet. A photo-<br />

graph of <strong>the</strong> sessile drop of NaF at 1025'C, taken<br />

during calibration work, is shown in Fig. 2.3.9.<br />

Sessile Drop of Waf ut 1025'<br />

PERfOD ENDING JUNE 10, 1956<br />

culated by using <strong>the</strong> tables of Bashforth and<br />

Adams12 and <strong>the</strong> densities obtained by Miles.13<br />

The initial experiments indicated no change in<br />

surface tension when an atmosphere of helium was<br />

admitted to <strong>the</strong> apparatus in which tests had been<br />

made under vacuum. When tests were conducted<br />

in vacuum, however, volatilization of ZrF, caused<br />

large changes in composition of <strong>the</strong> drop; helium<br />

atmospheres have been adopted as standard for<br />

future tests.<br />

Data typical of those obtained to date for<br />

NaF-ZrF, melts whose initial composition was<br />

53 mole % NaF and 47 mole % ZrF are shown in<br />

Table 2.3.4. While <strong>the</strong> data of &e earlier ex-<br />

periments are viewed with some uncertainty, <strong>the</strong><br />

relative agreement of <strong>the</strong> surface tension values<br />

obtained from droplets of widely varying sizes<br />

(as evidenced by <strong>the</strong> spread of sample weights<br />

and x/z ratios) is gratifying.<br />

SPECIFIC CONDUCTANCE AND DENSITY<br />

OF FUSED LITHIUM, POTASSIUM,<br />

AND CESIUM FLUORIDES"<br />

E. R. Van Artsdalen<br />

Electrical conductance and density have been<br />

measured as a function of temperature for pure,<br />

fused lithium, potassium, and cesium fluorides. A<br />

newly designed bridge, in conjunction with a<br />

special cell fabricated from platinum-rhodium<br />

alloy, was used in <strong>the</strong> measurements. The results<br />

of <strong>the</strong> measurements are expressed by <strong>the</strong><br />

equations listed in Tables 2.3.5 and 2.3.6. Similar<br />

data were also obtained for several rare-earth<br />

ons of <strong>the</strong> re-<br />

119

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