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CFD modeling of natural convection in pebble bed geometry with finite volume method

  • Salih Said Çatalbas ORCID logo and Ali Tiftikci ORCID logo EMAIL logo
Published/Copyright: October 9, 2023
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Abstract

In this study, we used the finite volume method to computationally model natural convective flow in packed bed geometry. Using the OpenFOAM® v2112 code, we performed the computational analysis. We successfully meshed the intricate packed bed flow geometry, which consists of several spheres positioned at random. The spheres have sizes of 0.006 and 0.01 m, and the associated Rayleigh numbers are 1.83 × 107 and 8.48 × 107 respectively. We used the packed bed heights of H/d = 5, 10, and 20 in the simulations. By comparing the results of the OpenFOAM® v2112 simulations of the natural convection flow for all self-heating sphere in a packed bed, we demonstrated that the velocity distributions and Nusselt values are in good agreement with the experimental data. Additionally, it was evident from the velocity and temperature distributions in a packed bed core that there was a major temperature rise at nearby low velocity fields and a minor velocity rise in the intermediate and upper elevations. We showed that increasing the height of the pebble-bed core and correspondingly increasing the quantity of spheres inside it makes the flow more difficult and also generates local hot spots. This study is notable for using the finite volume method to evaluate natural convection flow in all self-heating packed beds and for simulating packed bed flow using a significant number of spheres. These two factors contribute to the originality of this work.


Corresponding author: Ali Tiftikci, Nuclear Engineering Department, Faculty of Engineering and Architecture, Sinop University, Osmaniye Köyü Nasuhbaşoğlu Mevkii, 57000, Sinop, Türkiye, E-mail:

  1. Research ethics: Not applicable.

  2. Author contributions: The authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Competing interests: The authors states no conflict of interest.

  4. Research funding: This study was co-funded by the Scientific and Technological Research Council of Turkey (TUBITAK) ARDEB 2523 grant no 120N935 and by the Ministry of Science and ICT (MSIT) with National Research Foundation (NRF) (grant codes 2020K2A9A1A06097156).

  5. Data availability: The raw data can be obtained on request from the corresponding author.

Nomenclature

CFD

computational fluid dynamics

FVM

finite volume method

VHTR

very high temperature reactor

HTGR

high temperature gas-cooled reactor

FCC

face-centered cubic

BCC

body centered cubic

STL

standard tessellation language

CFL

Courant–Friedrichs–Lewy

PISO

pressure-implicit with splitting of operators

SIMPLE

semi-implicit method for pressure-linked equations

RANS

Reynolds-averaged Navier Stokes

DNS

direct numerical simulations

PDE

partial differential equations

Rad

Rayleigh number

Re

Reynolds number

Pr

Prandtl number

Nud

Nusselt number

k

mean value of turbulent kinetic energy

k max

maximum value of turbulent kinetic energy

u w

mean value of turbulent shear stress

u w max

maximum value of turbulent shear stress

H/d

height to sphere diameter ratio

U

z-velocity

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Received: 2023-05-20
Published Online: 2023-10-09
Published in Print: 2023-12-15

© 2023 Walter de Gruyter GmbH, Berlin/Boston

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