TY - JOUR
T1 - Effects of transverse power distribution on thermal hydraulic analysis
AU - Jo, Daeseong
AU - Seo, Chul Gyo
N1 - Publisher Copyright:
© 2015 Elsevier Ltd. All rights reserved.
PY - 2015/5
Y1 - 2015/5
N2 - To investigate the effects of transverse power distribution on fuel temperature, a two-dimensional thermal analysis model was developed in this study. An equilibrium reactor core with 22 fuel assemblies facilitated with plate-type fuel was modeled using Monte Carlo N-Particle (MCNP) code, and the fuel assembly that released the largest amount of power was obtained. The fuel plates were divided into 4 or 12 vertical stripes within the fuel width in order to obtain the transverse power distributions. With 4 stripes in the fuel, the highest power peaking was 2.36, whereas the highest power peaking was 2.70 with 12 stripes in the fuel. A 6th order polynomial was generated to predict the local power peaking at the edge of the fuel. Using this 6th order polynomial, the maximum power peaking at the edge of the fuel was 3.06. As per transverse power distributions, the temperature at the edge of the fuel should have been higher with a higher power peaking. However, the maximum temperature in the fuel decreased with a power peaking higher than 2.65. This was because the high power locally released from the edge of the fuel was immediately dissipated to the cladding by lateral heat conduction. As with the maximum temperature, the heat flux also overshot and converged at a certain value. This showed that the fuel did not need to be divided into more than 18 vertical stripes within the fuel width in order to obtain the local power peaking from nuclear physics calculations.
AB - To investigate the effects of transverse power distribution on fuel temperature, a two-dimensional thermal analysis model was developed in this study. An equilibrium reactor core with 22 fuel assemblies facilitated with plate-type fuel was modeled using Monte Carlo N-Particle (MCNP) code, and the fuel assembly that released the largest amount of power was obtained. The fuel plates were divided into 4 or 12 vertical stripes within the fuel width in order to obtain the transverse power distributions. With 4 stripes in the fuel, the highest power peaking was 2.36, whereas the highest power peaking was 2.70 with 12 stripes in the fuel. A 6th order polynomial was generated to predict the local power peaking at the edge of the fuel. Using this 6th order polynomial, the maximum power peaking at the edge of the fuel was 3.06. As per transverse power distributions, the temperature at the edge of the fuel should have been higher with a higher power peaking. However, the maximum temperature in the fuel decreased with a power peaking higher than 2.65. This was because the high power locally released from the edge of the fuel was immediately dissipated to the cladding by lateral heat conduction. As with the maximum temperature, the heat flux also overshot and converged at a certain value. This showed that the fuel did not need to be divided into more than 18 vertical stripes within the fuel width in order to obtain the local power peaking from nuclear physics calculations.
KW - Fuel temperature
KW - Plate type fuel
KW - Power peaking factor
KW - Thermal hydraulic analysis
KW - Transverse power
UR - http://www.scopus.com/inward/record.url?scp=84921300369&partnerID=8YFLogxK
U2 - 10.1016/j.pnucene.2014.12.017
DO - 10.1016/j.pnucene.2014.12.017
M3 - Article
AN - SCOPUS:84921300369
SN - 0149-1970
VL - 81
SP - 16
EP - 21
JO - Progress in Nuclear Energy
JF - Progress in Nuclear Energy
ER -