Abstract

The flow and heat transfer characteristics of the lead–bismuth eutectic (LBE) (Prandtl number Pr = 0.025) passing over a circular cylinder at Re = 500 are studied by direct numerical simulation and compared with the case of the air (Pr = 0.71). This article makes two major contributions: (1) heat transfer characteristics for the LBE flowing past a circular cylinder. For the case of air, the results show that a similarity exists among the wake structure of instantaneous temperature, fluctuating temperature, and velocity. However, these fields differ severely for the case of LBE. The local time-averaged Nusselt number (Nu¯) and circumferentially averagedNu¯are smaller in the LBE than that in the air. The circumferential and spanwise distributions ofNu¯in the LBE show a greater uniformity. The regions with larger circumferential or spanwise inhomogeneity appear in the flow separation zone. Besides, a resemblance between the distribution of the root mean square of fluctuation temperature and the turbulence kinetic energy can be recognized in the air; however, the similarity disappears for the case of LBE and in which the temperature fluctuation is smaller than that in the air. (2) Study on the temperature and velocity defect laws in the wake. By introducing the defect scales, it is concluded that the velocity field has not entered the self-preserving state yet, while the self-preserving state starts at the location of five times the diameter of the cylinder downstream of the cylinder for the temperature in the LBE and that of 21 times for the temperature in the air. In summary, even if without taking the buoyancy force into consideration, this article provides a fruitful description of the flow and heat transfer characteristics when the LBE flows past a cylinder, which is a typical flow in a helical coil steam generator of lead–bismuth alloy-cooled fast reactors. These highly resolved data on velocity and temperature are valuable for turbulence and heat fluxes modeling in the future and may facilitate the in-depth understanding of such flow and heat transfer characteristics within a limited variation range of operating temperature.

Highlights

  • As single-phase coolants with good performance, liquid metals are widely used in advanced nuclear reactor systems (Todreas and Kazim, 2011), chip cooling (Khalaj and Halgamuge, 2017; Muhammad et al, 2020), spallation particle sources (Batta et al, 2015), and other applications with extremely high heat loads

  • In a helical coil steam generator of an LFR system, lead–bismuth eutectic (LBE) in the shell side transfers the heat taken from the nuclear reactor core to the cooling water in the tube side, which makes it of great importance to analyze the flow and heat transfer behavior when LBE sweeps the tube bundle of the steam generator

  • The velocity and pressure relevant results are discussed regardless of Pr, as the temperature is considered as a passive scalar; that is, the heat transfer under different Pr has no effect on the flow field

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Summary

INTRODUCTION

As single-phase coolants with good performance, liquid metals are widely used in advanced nuclear reactor systems (Todreas and Kazim, 2011), chip cooling (Khalaj and Halgamuge, 2017; Muhammad et al, 2020), spallation particle sources (Batta et al, 2015), and other applications with extremely high heat loads. DNS is used in the simulation of forced and mixed convention in a backward-facing step under a uniform heat flux boundary condition for fluids with different Pr to study the influence of Pr on turbulent Pr (Prt) (Zhao et al, 2018). These studies have confirmed that the heat transfer characteristics of fluids with a low Pr are significantly different from those of fluids with Pr ~1. Researches on the flow and heat transfer characteristics of fluids with a low Pr by DNS focus on simple configurations such as a channel, backward-facing step, annular cavity, and pipes.

Problem Description
Numerical Schemes
Numerical Settings and Grid
Result
Instantaneous Fields and Vortex Structure
Nusselt Number
Characteristics of Temperature Field
Temperature and Velocity Defect Laws in Wake
Velocity Defect, Temperature Defect and Defect Width
Transverse Profiles and Fluctuation Attenuation
Summary As can be seen from Figure 12 and
CONCLUSION
DATA AVAILABILITY STATEMENT
Full Text
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