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ORNL-1816 - the Molten Salt Energy Technologies Web Site

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+<br />

a s<br />

b<br />

information <strong>the</strong> air flow rate and <strong>the</strong> <strong>the</strong>rmal re-<br />

were obtained as functions<br />

of <strong>the</strong> air pressure drop across <strong>the</strong> exchanger (<strong>the</strong><br />

steam-side resistance was negligible compared<br />

with <strong>the</strong> air-side resistance). Combination of<br />

<strong>the</strong>se data wi ed coefficients for <strong>the</strong><br />

fused salt, after allowance for difference in oper-<br />

ating temperatures, yielded performance curves for<br />

<strong>the</strong> exchanger under anticipated in-pile operating<br />

conditions, The data and a description of <strong>the</strong><br />

experiment are reported elsewhere.’ The method<br />

of conversion of <strong>the</strong> results of <strong>the</strong> experiment to<br />

in-pile conditions and <strong>the</strong> performance curves for<br />

<strong>the</strong> exchanger have been reported.2 A curve of<br />

<strong>the</strong> heat removal rate as a function of pressure<br />

drop of <strong>the</strong> in-pile loop heat exchanger is given<br />

N FLUIDS WITH<br />

HEAT SOURCES<br />

I Engineering Division<br />

The free-convection research, which had been<br />

’P. I. Perry, A. D. Rossin, and F. D. Miraldi, Mo-<br />

mentum und Heat Transfer Studies o an In-Ptle Loop<br />

Heat Exchanger, KT-174 (to be issued f .<br />

*M. W. Rosenthal, Performance of ANP In-Pile Loop<br />

Heat Exchanger, <strong>ORNL</strong> CF-54-9-83 (Sept. 10, 1954).<br />

PERIOD ENDING DECEMBER 10,7954<br />

however, more limited objectives than beiore. In<br />

<strong>the</strong> beginning of <strong>the</strong> <strong>ORNL</strong>-ANP effort, <strong>the</strong>re was<br />

no information on free convection in fluids with<br />

volume heat sources. Since <strong>the</strong> temperature struc-<br />

ture in <strong>the</strong> fuel pins of <strong>the</strong> first fused salt aircraft<br />

reactor experiment could not be readily predicted<br />

because of a lack of knowledge about <strong>the</strong> free-<br />

convection heat transfer in such a system, a<br />

free-convection research program was initiated.<br />

The principal objective was to determine both<br />

<strong>the</strong>oretically and experimentally <strong>the</strong> teriperature<br />

and velocity structure in a free-convection flat-<br />

plate system and, from <strong>the</strong>se data, to discover<br />

basic postulates that would permit analytical pre-<br />

diction of different systems which might be of<br />

interest in future fuel element designs. This<br />

project was well under way when <strong>the</strong> change to<br />

<strong>the</strong> present circulating-fuel reactor design was<br />

made. At that time <strong>the</strong> effort was greatly reduced,<br />

and later this research was temporarily abandoned<br />

in favor of more pressing problems. A series of<br />

memorandums summarizing <strong>the</strong> <strong>the</strong>oretical work<br />

which had been accomplished were prepared.<br />

AI so, some prel imi nary experimental velocity<br />

measurements in a flat-plate apparatus were ob-<br />

tained.<br />

In <strong>the</strong> intervening years <strong>the</strong>re has been a con-<br />

tinued interest in <strong>the</strong> temperature structure in<br />

fluids with volume heat sources that art: losing<br />

heat by free convection in applications such as<br />

dump tanks for liquid fuel reactors, radiation<br />

damage capsules, and pins containing Iiqluid fuel.<br />

The repeated queries on this subject prompted<br />

<strong>the</strong> decision to reactivate <strong>the</strong> research, but on a<br />

less ambitious basis than before. Hence, (3 report3<br />

y which provides a wider<br />

distribution to <strong>the</strong> <strong>the</strong>oretical analyses which were<br />

distributed locally as me s in 1951 and<br />

coefficient) for a modified version of <strong>the</strong> flat-plate<br />

svstem in which it will not be nece:jsary to

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