Cryogenic thermal analysis of the HANARO cold neutron moderator cell

Author(s):  
Gee Y. Han ◽  
Kye H. Lee ◽  
Heonil Kim
Author(s):  
M. V. Bulavin ◽  
A. A. Belyakov ◽  
A. E. Verkhoglyadov ◽  
S. A. Kulikov ◽  
K. A. Mukhin

2017 ◽  
Vol 14 (3) ◽  
pp. 520-532
Author(s):  
M. V. Bulavin ◽  
A. V. Kazakov ◽  
E. P. Shabalin

2000 ◽  
Vol 276-278 ◽  
pp. 214-215 ◽  
Author(s):  
T. Grósz ◽  
T. Hargitai ◽  
V.A. Mityukhlyaev ◽  
L. Rosta ◽  
A.P. Serebrov ◽  
...  

2002 ◽  
Vol 311 (1-2) ◽  
pp. 164-172 ◽  
Author(s):  
Takeshi Kawai ◽  
Hirofumi Yoshino ◽  
Yuji Kawabata ◽  
Masahiro Hino ◽  
Chien-Hsiung Lee ◽  
...  

2018 ◽  
Vol 551 ◽  
pp. 377-380
Author(s):  
T. Cronert ◽  
J.P. Dabruck ◽  
M. Klaus ◽  
C. Lange ◽  
P. Zakalek ◽  
...  

2012 ◽  
Vol 50 ◽  
pp. 1-7 ◽  
Author(s):  
Shuo Sun ◽  
Yuntao Liu ◽  
Hongli Wang ◽  
Dongfeng Chen ◽  
Quanke Feng ◽  
...  

2015 ◽  
Vol 12 (6) ◽  
pp. 773-777 ◽  
Author(s):  
A. Belyakov ◽  
M. Bulavin ◽  
A. Chernikov ◽  
A. Churakov ◽  
S. Kulikov ◽  
...  

2016 ◽  
Vol 2016 ◽  
pp. 1-11
Author(s):  
Mark Ho ◽  
Yeongshin Jeong ◽  
Haneol Park ◽  
Guan Heng Yeoh ◽  
Weijian Lu

The cold neutron source (CNS) system of the Open Pool Australian Light-Water (OPAL) reactor is a 20 L cryogenically cooled liquid deuterium thermosiphon system. The CNS is cooled by forced convective helium which is held at room temperature during stand-by (SO) mode and at ~20 K during normal operation (NO) mode. When helium cooling stops, the reactor is shut down to prevent the moderator cell from overheating. This computational fluid dynamics (CFD) study aims to determine whether the combined effects of conduction and natural convection would provide sufficient cooling for the moderator cell under the influence of reactor decay heat after reactor shutdown. To achieve this, two commercial CFD software packages using an identical CFD mesh were first assessed against an experimental heat transfer test of the CNS. It was found that both numerical models were valid within the bounds of experimental uncertainty. After this, one CFD model was used to simulate the thermosiphon transient condition after the reactor is shut down. Two independent shutdown conditions of different decay-heat power profiles were simulated. It was found that the natural convection and conduction cooling in the thermosiphon were sufficient for dissipating both decay-heat profiles, with the moderator cell remaining below the safe temperature of 200°C.


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