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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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