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 />
Three of <strong>the</strong> capsules were exposed to 1.1 x 1017<br />
t,,,. Gray-green solid residues which filled as<br />
much as 90% of <strong>the</strong> volume were found in all <strong>the</strong><br />
capsules. The residues in <strong>the</strong> capsules exposed<br />
o a flux of 1.1 x 1017 analyzed 92% uranium, and<br />
he residues in those exposed to a flux of 2.0 x<br />
10'' analyzed 24% uranium. In <strong>the</strong> capsules given<br />
e higher exposure, gas pressures of between 55<br />
and 100 psi developed. Analyses of <strong>the</strong>se gases<br />
showed about 30% CF, and about 25% C,F,; <strong>the</strong><br />
remaining gas was unidentified,<br />
MINIATURE IN-PILE LOOP<br />
Bench Test<br />
W. R. Willis<br />
M. F. Osborne<br />
H. E. Robertson G. W. Keilholtz<br />
Solid State Division<br />
irst successful bench test of <strong>the</strong> miniature<br />
in-pile loop designed for insertion in a vertical<br />
hole in <strong>the</strong> LITR included four freezing and melting<br />
cycles in 260 hr of operation. The loop was oper-<br />
ated at 1466OF. The linear velocity of <strong>the</strong> fused<br />
salt circulated in <strong>the</strong> loop was between 3.3 fps<br />
(as calculated from <strong>the</strong> flowmeter) and 3.8 fps (as<br />
calculated from <strong>the</strong> pump speed); thus a Reynolds<br />
number of about 3000 was obtained. Since it was<br />
possible to freeze and melt <strong>the</strong> fused salt without<br />
causing failure of <strong>the</strong> loop, it may be advisable to<br />
fill <strong>the</strong> in-pile loop before it is inserted in <strong>the</strong><br />
reactor and <strong>the</strong>n melt <strong>the</strong> fuel mixture after <strong>the</strong><br />
loop is in position. Since, during <strong>the</strong> bench test,<br />
<strong>the</strong> flowmeter was found to be temperature sensitive,<br />
<strong>the</strong> dependence of <strong>the</strong> measurement on <strong>the</strong> temper-<br />
ature must be established.<br />
The bench test was terminated because of a leak<br />
in a collar that was welded over a joint in <strong>the</strong> fuel<br />
tube. The two ends of <strong>the</strong> loop did not butt toge<strong>the</strong>r<br />
at this location, and <strong>the</strong> annular space thus formed<br />
between <strong>the</strong> collar and <strong>the</strong> tube sections trapped<br />
<strong>the</strong> fused salt in such a manner that expansion of<br />
<strong>the</strong> salt caused <strong>the</strong> collar (not <strong>the</strong> weld) to rupture.<br />
The metal collar stretched from 0.4 in. in diameter<br />
to 0.5 in, before it ruptured, The salt from <strong>the</strong><br />
leak, which existed during operation for about 4<br />
hr, showed a tendency to oxidize and to stick to<br />
<strong>the</strong> lnconel surface ra<strong>the</strong>r than to flow rapidly down<br />
<strong>the</strong> outside tube wall. Thus, a leak in <strong>the</strong> colder<br />
portion of a loop that was operating in-pile would<br />
probably not flow downward into <strong>the</strong> high-flux<br />
region before a safety alarm from <strong>the</strong> released<br />
radioactivity could scram <strong>the</strong> reactor.<br />
A Delco motor from <strong>the</strong> group being used in bench<br />
tests has been rebuilt to withstand radiation and<br />
a higher temperature. The wire on both <strong>the</strong> rotor<br />
and <strong>the</strong> stator was replaced with glass-insulated<br />
wire, 411 paper was removed, and mica was used<br />
in <strong>the</strong> commutator and in <strong>the</strong> rotor segments; glass<br />
cloth yas used, where possible, for o<strong>the</strong>r insula-<br />
tion. These changes required that <strong>the</strong> shaft as-<br />
sembly be slightly modified to allow more space<br />
for windings. The rebuilt motor was tested during<br />
<strong>the</strong> bench test of <strong>the</strong> miniature loop, and it was found<br />
to be satisfactory, In a comparison of <strong>the</strong> operation<br />
of <strong>the</strong> rebuilt motor with that of <strong>the</strong> original motor<br />
under no load and under load conditions, <strong>the</strong> rebuilt<br />
motor was found to be slightly more efficient than<br />
<strong>the</strong> original motor. Fur<strong>the</strong>rmore, since <strong>the</strong> rebuilt<br />
motor can withstand a higher ambient temperature<br />
and since for a given voltage it produces a higher<br />
speed, higher fuel velocities can be obtained than<br />
were possible previously.<br />
Heat Transfer Calculations<br />
M. T. Robinson<br />
Solid State Division<br />
E. R. Mann F. P. Green<br />
R. S. Stone<br />
Instrumentation and Controls Division<br />
D. F. Weekes, Consultant<br />
An extensive series of heat transfer calculations<br />
has been carried out on <strong>the</strong> <strong>ORNL</strong> Reactor Controls<br />
Computer in order to predict <strong>the</strong> <strong>the</strong>rmal behavior<br />
of a miniature in-pile circulating-fuel loop. The<br />
derivations of appropriate differential equations<br />
and <strong>the</strong> details of <strong>the</strong>ir solution are given in a<br />
forthcoming report,2 The model finally adopted for<br />
<strong>the</strong> calculations and for <strong>the</strong> in-pile loop is shown in<br />
Fig. 9.2. It was assumed to be mounted in position<br />
C-48 of <strong>the</strong> LITR, with <strong>the</strong> lower end at <strong>the</strong> location<br />
of maximum <strong>the</strong>rmal-neutron flux.3 The maximum<br />
power density in <strong>the</strong> fuel in position C-48 was<br />
assumed to be 540 w/cm3.<br />
The computer results were obtained for a variety<br />
of different flow rates of fuel (NaF-ZrF,-UF,,<br />
53.5-40-6.5 mole %) and of cooling air expressed<br />
as Reynolds number of <strong>the</strong> cooling air stream, Re,<br />
or fuel stream, Re The heat transfer, y, that is,<br />
f'<br />
*M. T. Robinson and D. F. Weekes, Design Calculation<br />
for Miniature Hi h Temperature In-Pile Circulating<br />
Fuel Loop, <strong>ORNL</strong>-1888 (' in press).<br />
3M. T. Robinson, Solid State Semiann. Prog. Rep.<br />
Feb. 28, 1954, <strong>ORNL</strong>-1677, p 27.