Void fraction distribution in a rod bundle with part-length rods via high-energy X-ray computed tomography

The void fraction distribution of a fuel rod bundle in a boiling water reactor is a critical parameter for accurately predicting the optimal thermal margin in the design of a reactor core. The rod bundle configuration, such as a part-length rod (PLR) and water rod, can affect void distribution. To c...

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Autores principales: Takahiro ARAI, Atsushi UI, Masahiro FURUYA, Riichiro OKAWA, Tsugumasa IIYAMA, Shota UEDA, Kenetsu SHIRAKAWA, Kazuaki KITO
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Publicado: The Japan Society of Mechanical Engineers 2021
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spelling oai:doaj.org-article:06c6b44fd39c42b1aeae9ba64afff1dc2021-11-29T06:09:58ZVoid fraction distribution in a rod bundle with part-length rods via high-energy X-ray computed tomography2187-974510.1299/mej.21-00001https://doaj.org/article/06c6b44fd39c42b1aeae9ba64afff1dc2021-05-01T00:00:00Zhttps://www.jstage.jst.go.jp/article/mej/8/4/8_21-00001/_pdf/-char/enhttps://doaj.org/toc/2187-9745The void fraction distribution of a fuel rod bundle in a boiling water reactor is a critical parameter for accurately predicting the optimal thermal margin in the design of a reactor core. The rod bundle configuration, such as a part-length rod (PLR) and water rod, can affect void distribution. To clarify the influence of PLR on void fraction distribution, a boiling flow experiment was conducted using a 5 × 5 heated rod bundle that partially simulated a boiling water reactor (BWR) rod bundle, and three PLRs were arranged in the corner. The cross-sectional void fraction distribution was acquired using high-energy X-ray computed tomography at six height levels for wide flow conditions, system pressures of 0.1 − 7.2 MPa, inlet subcoolings of 20 - 90 kJ/kg, mass fluxes of 500 - 1250 kg/m2/s, and linear heat generation rates (LHGR) of 3.2 - 8.6 kW/m. In the PLR region, the local void fraction temporarily decreases because the PLRs disappear, and the flow channel rapidly expands. Together with the downstream PLRs, the voids propagate to the PLR region and concentrate in the center. The void fraction in the corner of the PLR region remains lower. A maximum 26% decrease in the subchannel void fraction was observed in the corner of the PLR region at the system pressure of 7.2 MPa, mass flux of 1.25 × 103 kg/m2/s, inlet subcooling of 50 kJ/kg, and LHGR of 8.6 kW/m.Takahiro ARAIAtsushi UIMasahiro FURUYARiichiro OKAWATsugumasa IIYAMAShota UEDAKenetsu SHIRAKAWAKazuaki KITOThe Japan Society of Mechanical Engineersarticle5 × 5 rod bundlevoid fraction distributionboiling two-phase flowlinear accelerator-driven high-energy x-ray computed tomographypart-length rodMechanical engineering and machineryTJ1-1570ENMechanical Engineering Journal, Vol 8, Iss 4, Pp 21-00001-21-00001 (2021)
institution DOAJ
collection DOAJ
language EN
topic 5 × 5 rod bundle
void fraction distribution
boiling two-phase flow
linear accelerator-driven high-energy x-ray computed tomography
part-length rod
Mechanical engineering and machinery
TJ1-1570
spellingShingle 5 × 5 rod bundle
void fraction distribution
boiling two-phase flow
linear accelerator-driven high-energy x-ray computed tomography
part-length rod
Mechanical engineering and machinery
TJ1-1570
Takahiro ARAI
Atsushi UI
Masahiro FURUYA
Riichiro OKAWA
Tsugumasa IIYAMA
Shota UEDA
Kenetsu SHIRAKAWA
Kazuaki KITO
Void fraction distribution in a rod bundle with part-length rods via high-energy X-ray computed tomography
description The void fraction distribution of a fuel rod bundle in a boiling water reactor is a critical parameter for accurately predicting the optimal thermal margin in the design of a reactor core. The rod bundle configuration, such as a part-length rod (PLR) and water rod, can affect void distribution. To clarify the influence of PLR on void fraction distribution, a boiling flow experiment was conducted using a 5 × 5 heated rod bundle that partially simulated a boiling water reactor (BWR) rod bundle, and three PLRs were arranged in the corner. The cross-sectional void fraction distribution was acquired using high-energy X-ray computed tomography at six height levels for wide flow conditions, system pressures of 0.1 − 7.2 MPa, inlet subcoolings of 20 - 90 kJ/kg, mass fluxes of 500 - 1250 kg/m2/s, and linear heat generation rates (LHGR) of 3.2 - 8.6 kW/m. In the PLR region, the local void fraction temporarily decreases because the PLRs disappear, and the flow channel rapidly expands. Together with the downstream PLRs, the voids propagate to the PLR region and concentrate in the center. The void fraction in the corner of the PLR region remains lower. A maximum 26% decrease in the subchannel void fraction was observed in the corner of the PLR region at the system pressure of 7.2 MPa, mass flux of 1.25 × 103 kg/m2/s, inlet subcooling of 50 kJ/kg, and LHGR of 8.6 kW/m.
format article
author Takahiro ARAI
Atsushi UI
Masahiro FURUYA
Riichiro OKAWA
Tsugumasa IIYAMA
Shota UEDA
Kenetsu SHIRAKAWA
Kazuaki KITO
author_facet Takahiro ARAI
Atsushi UI
Masahiro FURUYA
Riichiro OKAWA
Tsugumasa IIYAMA
Shota UEDA
Kenetsu SHIRAKAWA
Kazuaki KITO
author_sort Takahiro ARAI
title Void fraction distribution in a rod bundle with part-length rods via high-energy X-ray computed tomography
title_short Void fraction distribution in a rod bundle with part-length rods via high-energy X-ray computed tomography
title_full Void fraction distribution in a rod bundle with part-length rods via high-energy X-ray computed tomography
title_fullStr Void fraction distribution in a rod bundle with part-length rods via high-energy X-ray computed tomography
title_full_unstemmed Void fraction distribution in a rod bundle with part-length rods via high-energy X-ray computed tomography
title_sort void fraction distribution in a rod bundle with part-length rods via high-energy x-ray computed tomography
publisher The Japan Society of Mechanical Engineers
publishDate 2021
url https://doaj.org/article/06c6b44fd39c42b1aeae9ba64afff1dc
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