Experimental study of flow field and transition characteristics in rod bundle channel

• Published in: Annals of nuclear energy Vol. 193; p. 110056
• Main Authors: Qi, Peiyao, Han, Chuangao, Ma, Chen, Zhang, Ruixiang, Liu, Feng, SichaoTan
• Format: Journal Article
• Language: English
• Published: Elsevier Ltd 01.12.2023
• Subjects: Flow resistance; PIV; Rod bundle; Transition; Turbulence characteristics; Turbulence characteristics; Transition; Flow resistance; PIV; Rod bundle
• ISSN: 0306-4549; 1873-2100
• DOI: 10.1016/j.anucene.2023.110056

•PIV used to study flow fields & turbulence in 5x5 rod bundle across 22 cases (Reynolds: 310-12296).•Higher turbulence intensity at lower Reynolds due to significant relative velocity gradient in rod bundle.•Transition Reynolds ≈ 900 in rod bundle, less distinct than in pipes.•Fluctuation velocity decreases with Reynolds, abrupt rise at transition Reynolds.•Non-uniform transition Reynolds leads to varying turbulence intensity in rod bundle. Utilizing the particle image velocimetry (PIV) technique, this study investigates the fully developed flow field and turbulence statistics in a 5×5 rod bundle across 22 cases, with Reynolds numbers ranging from 310 to 12296.Time-averaged, statistical, and spectral analyses were performed on the full field and instantaneous velocity vectors obtained through PIV measurements to examine the velocity distribution, turbulence characteristics, and spectral features in different subchannels under various Reynolds numbers. In conjunction with a differential pressure transmitter, the flow properties and fluid transitions were also explored.The experimental results reveal that the relative velocity gradient in the rod bundle channel is more significant at lower Reynolds numbers. As the Reynolds number increases, the relative velocity distribution becomes more uniform. A comparison of experimental results from different planes indicates that the fluctuation velocity in the gap subchannel is greater than that in the inner subchannel, suggesting that tightly arranged rods can generate higher turbulence intensity. Furthermore, the transition observed through the friction factor in the rod bundle channel is less distinct than those in pipes, with the transition Reynolds number being approximately 900. A low Reynolds number effect is present in the rod bundle channel, where the dimensionless fluctuation velocity decreases as the Reynolds number increases. Upon reaching the transition Reynolds number, the area-averaged dimensionless fluctuation velocity abruptly rises. By examining the turbulence intensity variations at different positions within the rod bundle, it becomes evident that the transition Reynolds numbers vary across different subchannel positions. Ultimately, the experimental data can be employed to validate the applicability of turbulence models for different Reynolds numbers.