Large-eddy simulation of thermal fatigue in a mixing tee

Temperature fluctuations occur due to thermal mixing of hot and cold streams in the T-junctions of the piping system in nuclear power plants, which may cause thermal fatigue of piping system. In this paper, three-dimensional, unsteady numerical simulations of coolant temperature fluctuations at a mi...

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Main Authors: Ming, Tingzhen., Zhao, Jiyun.
Other Authors: School of Electrical and Electronic Engineering
Format: Article
Language:English
Published: 2013
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Online Access:https://hdl.handle.net/10356/85057
http://hdl.handle.net/10220/11534
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-850572020-03-07T13:57:24Z Large-eddy simulation of thermal fatigue in a mixing tee Ming, Tingzhen. Zhao, Jiyun. School of Electrical and Electronic Engineering DRNTU::Engineering::Electrical and electronic engineering Temperature fluctuations occur due to thermal mixing of hot and cold streams in the T-junctions of the piping system in nuclear power plants, which may cause thermal fatigue of piping system. In this paper, three-dimensional, unsteady numerical simulations of coolant temperature fluctuations at a mixing T-junction of equal diameter pipes were performed using the large eddy simulation (LES) turbulent model. The experiments used in this paper to benchmark the simulations were performed by Hitachi Ltd. The calculated normalized mean temperatures and fluctuating temperatures are in good agreement with the measurements. The influence of the time-step ranging from 100 Hz to 1000 Hz on the numerical simulation results was explored. The simulation results indicate that all the results with different frequencies agree well with the experimental data. Finally, the attenuation of fluctuation of fluid temperature was also investigated. It is found that, drastic fluctuation occurs within the range of less than L/D = 4.0; the fluctuation of fluid temperature does not always attenuate from the pipe center to the wall due to the continuous generation of vortexes. At the top wall, the position of L/D = 1.5 has a minimum normalized mean temperature and a peak value of root-mean square temperature, whereas at the bottom wall, the position having the same characteristics is L/D = 2.0. 2013-07-16T03:57:56Z 2019-12-06T15:56:22Z 2013-07-16T03:57:56Z 2019-12-06T15:56:22Z 2012 2012 Journal Article Ming, T., & Zhao, J. (2012). Large-eddy simulation of thermal fatigue in a mixing tee. International Journal of Heat and Fluid Flow, 37, 93-108. 0142-727X https://hdl.handle.net/10356/85057 http://hdl.handle.net/10220/11534 10.1016/j.ijheatfluidflow.2012.06.002 en International journal of heat and fluid flow © 2012 Elsevier Inc.
institution Nanyang Technological University
building NTU Library
country Singapore
collection DR-NTU
language English
topic DRNTU::Engineering::Electrical and electronic engineering
spellingShingle DRNTU::Engineering::Electrical and electronic engineering
Ming, Tingzhen.
Zhao, Jiyun.
Large-eddy simulation of thermal fatigue in a mixing tee
description Temperature fluctuations occur due to thermal mixing of hot and cold streams in the T-junctions of the piping system in nuclear power plants, which may cause thermal fatigue of piping system. In this paper, three-dimensional, unsteady numerical simulations of coolant temperature fluctuations at a mixing T-junction of equal diameter pipes were performed using the large eddy simulation (LES) turbulent model. The experiments used in this paper to benchmark the simulations were performed by Hitachi Ltd. The calculated normalized mean temperatures and fluctuating temperatures are in good agreement with the measurements. The influence of the time-step ranging from 100 Hz to 1000 Hz on the numerical simulation results was explored. The simulation results indicate that all the results with different frequencies agree well with the experimental data. Finally, the attenuation of fluctuation of fluid temperature was also investigated. It is found that, drastic fluctuation occurs within the range of less than L/D = 4.0; the fluctuation of fluid temperature does not always attenuate from the pipe center to the wall due to the continuous generation of vortexes. At the top wall, the position of L/D = 1.5 has a minimum normalized mean temperature and a peak value of root-mean square temperature, whereas at the bottom wall, the position having the same characteristics is L/D = 2.0.
author2 School of Electrical and Electronic Engineering
author_facet School of Electrical and Electronic Engineering
Ming, Tingzhen.
Zhao, Jiyun.
format Article
author Ming, Tingzhen.
Zhao, Jiyun.
author_sort Ming, Tingzhen.
title Large-eddy simulation of thermal fatigue in a mixing tee
title_short Large-eddy simulation of thermal fatigue in a mixing tee
title_full Large-eddy simulation of thermal fatigue in a mixing tee
title_fullStr Large-eddy simulation of thermal fatigue in a mixing tee
title_full_unstemmed Large-eddy simulation of thermal fatigue in a mixing tee
title_sort large-eddy simulation of thermal fatigue in a mixing tee
publishDate 2013
url https://hdl.handle.net/10356/85057
http://hdl.handle.net/10220/11534
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