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
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
ANP QUARTERLY PROGRESS REPORT<br />
conduit shaped around a 9-in. core. After removal<br />
of <strong>the</strong> core, <strong>the</strong> ducts were stiffened by Fiberglas<br />
wrapping. The projected length of each duct along<br />
<strong>the</strong> z axis was 46.5 in., and <strong>the</strong> duct arrays were<br />
arranged so that <strong>the</strong>re was 5 in. between <strong>the</strong> duct<br />
center I ines.<br />
Thermal-neutron measurements beyond a single<br />
duct and a 3-duct array in a water medium were<br />
reported previously.6 Measurements made beyond<br />
<strong>the</strong> 35-duct array in both a water medium and a<br />
gamma-shield medium are shown in Fig. 13.6. The<br />
gamma shield consisted of steel Raschig rings<br />
(35 vol %) and water borated to 1% by volume.<br />
For both mediums <strong>the</strong> array was contained in a<br />
4-ft-long iron tank (t-in.-thick walls) which had<br />
'/,-in.-thick iron windows in each end. The<br />
windows were 29 in. in diameter and were slightly<br />
Fig. 13.6. Thermal-Neutron Flux Beyond Various<br />
Arrays of GE-ANP Helical Air Ducts (3 in. in<br />
Diameter, 46.5 in. Long).<br />
1 54<br />
larger than, and concentric with, <strong>the</strong> LTSF source<br />
plate. The measurements were made behind <strong>the</strong><br />
tank in <strong>the</strong> LTSF water.<br />
As indicated in Fig. 13.6, <strong>the</strong> presence of <strong>the</strong><br />
35 ducts in <strong>the</strong> gamma shield increased <strong>the</strong><br />
<strong>the</strong>rmal-neutron flux by a factor of approximately<br />
3000. In <strong>the</strong> medium of plain water, <strong>the</strong> flux was<br />
increased by a factor of 300. For <strong>the</strong> water<br />
medium <strong>the</strong> increase in flux seems to be consistent<br />
with a calculation which takes into account only<br />
<strong>the</strong> reduced density of <strong>the</strong> attenuating medium.<br />
For <strong>the</strong> case in which <strong>the</strong> ducts were in <strong>the</strong> gamma<br />
shield, <strong>the</strong> neutron streaming in <strong>the</strong> ducts appears<br />
to be relatively more important. The latter is not<br />
surprising, since <strong>the</strong> addition of <strong>the</strong> steel in-<br />
creases <strong>the</strong> attenuation of <strong>the</strong> medium to neutrons<br />
as well as to gamma rays.<br />
The fast-neutron dose rates beyond <strong>the</strong> 35-duct<br />
array both in a medium of water and in <strong>the</strong> Raschig<br />
ring-borated water medium are shown in Fig. 13.7.<br />
The gamma-ray dose rate beyond <strong>the</strong> gamma shield<br />
without <strong>the</strong> ducts is compared in Fig. 13.8 with<br />
that beyond <strong>the</strong> shield with <strong>the</strong> 35 ducts. The<br />
presence of <strong>the</strong> ducts increased <strong>the</strong> gamma dose<br />
rate by a factor of approximately 160.<br />
2<br />
10-2<br />
Fig. 13.7. Fast-Neutron Dose Rate Beyond 35<br />
GE-ANP Helical Air Ducts (3 in. in Diameter,<br />
46.5 in. Long).<br />
\<br />
\,<br />
,<br />
9 .<br />
. t<br />
/c<br />
E<br />
w