Thermal diffusivity and prandtl number of liquid mercury and potassium from melting point to critical point

1969 ◽  
Vol 31 (5) ◽  
pp. 1289-1301 ◽  
Author(s):  
A.V. Grosse
2021 ◽  
pp. 113276
Author(s):  
Junshuai Chen ◽  
Hongwei Xing ◽  
Taotao Zhan ◽  
Libin Chen ◽  
Maogang He ◽  
...  

2009 ◽  
Vol 30 (5) ◽  
pp. 1453-1465 ◽  
Author(s):  
J. V. Sengers ◽  
R. A. Perkins ◽  
M. L. Huber ◽  
B. Le Neindre

2021 ◽  
Vol 907 (1) ◽  
pp. 56
Author(s):  
Ambrish Pandey ◽  
Jörg Schumacher ◽  
Katepalli R. Sreenivasan

Author(s):  
Jonathan K. Lai ◽  
Elia Merzari ◽  
Yassin A. Hassan ◽  
Aleksandr Obabko

Abstract Difficulty in capturing heat transfer characteristics for liquid metals is commonplace because of their low molecular Prandtl number (Pr). Since these fluids have very high thermal diffusivity, the Reynolds analogy is not valid and creates modeling difficulties when assuming a turbulent Prandtl number (Prt) of near unity. Baseline problems have used direct numerical simulations (DNS) for the channel flow and backward facing step to aid in developing a correlation for Prt. More complex physics need to be considered, however, since correlation accuracy is limited. A tight lattice square rod bundle has been chosen for DNS benchmarking because of its presence of flow oscillations and coherent structures even with a relatively simple geometry. Calculations of the Kolmogorov length and time scales have been made to ensure that the spatial-temporal discretization is sufficient for DNS. In order to validate the results, Hooper and Wood’s 1984 experiment has been modeled with a pitch-to-diameter (P/D) ratio of 1.107. The present work aims at validating first- and second-order statistics for the velocity field, and then analyzing the heat transfer behavior at different molecular Pr. The effects of low Pr flow are presented to demonstrate how the normalized mean and fluctuating heat transfer characteristics vary with different thermal diffusivity. Progress and future work toward creating a full DNS database for liquid metals are discussed.


1997 ◽  
Vol 353 ◽  
pp. 45-66 ◽  
Author(s):  
I. A. ELTAYEB ◽  
D. E. LOPER

This is the final part of a three-part study of the stability of vertically oriented double-diffusive interfaces having an imposed vertical stable temperature gradient. In this study, flow is forced within a fluid of infinite extent by a prescribed excess of compositionally buoyant material within a circular cylindrical interface. Compositional diffusivity is ignored while thermal diffusivity and viscosity are finite. The instability of the interface is determined by quantifying the exponential growth rate of a harmonic deflection of infinitesimal amplitude. Attention is focused on the zonal wavenumber of the fastest growing mode.The interface is found to be unstable for some wavenumber for all values of the Prandtl number and interface radius. The zonal wavenumber of the fastest growing mode increases roughly linearly with interface radius, except for small values of the Prandtl number (<0.065). For small and moderate values of the radius, the preferred mode is either axisymmetric or has zonal wavenumber of 1, representing a helical instability. The growth rate of the fastest-growing mode is largest for interfaces having radii of from 2 to 3 salt-finger lengths.


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