Abstract

Using complementary experiments and direct numerical simulations, we study turbulent thermal convection of a liquid metal (Prandtl number $\textit {Pr}\approx 0.03$ ) in a box-shaped container, where two opposite square sidewalls are heated/cooled. The global response characteristics like the Nusselt number ${\textit {Nu}}$ and the Reynolds number $\textit {Re}$ collapse if the side height $L$ is used as the length scale rather than the distance $H$ between heated and cooled vertical plates. These results are obtained for various Rayleigh numbers $5\times 10^3\leq {\textit {Ra}}_H\leq 10^8$ (based on $H$ ) and the aspect ratios $L/H=1, 2, 3$ and $5$ . Furthermore, we present a novel method to extract the wind-based Reynolds number, which works particularly well with the experimental Doppler-velocimetry measurements along vertical lines, regardless of their horizontal positions. The extraction method is based on the two-dimensional autocorrelation of the time–space data of the vertical velocity.

Highlights

  • The understanding of turbulent thermal convection is of great importance for astrophysics, geophysics, climate research and engineering purposes alike

  • We will present the results and discuss the evidence, that the relevant length scale in vertical convection (VC) is based on the plate size rather than on the distance between the hot and cold plates

  • We studied VC of a liquid metal with low Prandtl number (Pr ≈ 0.03), more precisely, the eutectic alloy GaInSn, using the complementary results from experimental measurements and direct numerical simulations (DNS)

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Summary

Introduction

The understanding of turbulent thermal convection is of great importance for astrophysics, geophysics, climate research and engineering purposes alike. Convection has been under investigation for centuries, even today researchers struggle to unveil its complex nature. To study turbulent thermal convection, a model system is considered, where the fluid is confined between horizontal plates heated from below and cooled from above, commonly known as Rayleigh–Bénard convection (RBC) (Bodenschatz, Pesch & Ahlers 2000; Ahlers, Grossmann & Lohse 2009; Chillà & Schumacher 2012). In this work we study a different model system, where the fluid 932 A9-1. L. Zwirner and others is confined between vertical heated/cooled plates, known as convection inside a differentially heated enclosure, side-heated convection or vertical convection. Throughout this work, we will refer to this system as vertical convection (VC)

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