Analysis of Thermal Performances in a Ventilated Room Using LBM-MRT: Effect of a Porous Separation

This article demonstrates the feasibility of porous separation on the performance of displacement ventilation in a rectangular enclosure. A jet of fresh air enters the cavity through an opening at the bottom of the left wall and exits through an opening at the top of the right wall. The porous separ...

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Main Authors: Zouhira Hireche, Nabil Himrane, Lyes Nasseri, Yasmine Hamrioui, Djamel Eddine Ameziani
Format: Article
Language:English
Published: MDPI AG 2022-01-01
Series:Computation
Subjects:
Online Access:https://www.mdpi.com/2079-3197/10/1/4
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author Zouhira Hireche
Nabil Himrane
Lyes Nasseri
Yasmine Hamrioui
Djamel Eddine Ameziani
author_facet Zouhira Hireche
Nabil Himrane
Lyes Nasseri
Yasmine Hamrioui
Djamel Eddine Ameziani
author_sort Zouhira Hireche
collection DOAJ
description This article demonstrates the feasibility of porous separation on the performance of displacement ventilation in a rectangular enclosure. A jet of fresh air enters the cavity through an opening at the bottom of the left wall and exits through an opening at the top of the right wall. The porous separation is placed in the center of the cavity and its height varies between 0.2 and 0.8 with three values of thickness, 0.1, 0.2, and 0.3. The heat transfer rate was calculated for different intervals of Darcy (10<sup>−6</sup> ≤ Da ≤ 10), Rayleigh (10 ≤ Ra ≤ 10<sup>6</sup>), and Reynolds (50 ≤ Re ≤ 500) numbers. The momentum and the energy equations were solved by the lattice Boltzmann method with multiple relaxation times (LB-MRT). Schemes D2Q9 and D2Q5 were chosen for the velocity and temperature fields, respectively. For porous separation, the generalized Darcy–Brinkman–Forchheimer model was adopted. It is represented by a term added in the standard LB equations. For the dynamic domain, numerical simulations revealed complex flow structures depending on all control parameters. The results showed that the thermal field, mainly in the second compartment, is very dependent on the size and permeability of the porous separation. However, they have no influence on the transfer rate.
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spelling doaj.art-7896a18a660b4f9ebb656bb19677e72f2023-11-23T13:23:14ZengMDPI AGComputation2079-31972022-01-01101410.3390/computation10010004Analysis of Thermal Performances in a Ventilated Room Using LBM-MRT: Effect of a Porous SeparationZouhira Hireche0Nabil Himrane1Lyes Nasseri2Yasmine Hamrioui3Djamel Eddine Ameziani4Laboratory of Multiphase Transport and Porous Media (LTPMP), Faculty of Mechanical and Proceeding Engineering, University of Sciences and Technology Houari Boumediene, Algiers 16111, AlgeriaLaboratory of Energy and Mechanical Engineering (LEMI), Faculty of Technology, University of M’Hamed Bougara Boumerdes, Boumerdes 35000, AlgeriaLaboratory of Multiphase Transport and Porous Media (LTPMP), Faculty of Mechanical and Proceeding Engineering, University of Sciences and Technology Houari Boumediene, Algiers 16111, AlgeriaLaboratory of Multiphase Transport and Porous Media (LTPMP), Faculty of Mechanical and Proceeding Engineering, University of Sciences and Technology Houari Boumediene, Algiers 16111, AlgeriaLaboratory of Multiphase Transport and Porous Media (LTPMP), Faculty of Mechanical and Proceeding Engineering, University of Sciences and Technology Houari Boumediene, Algiers 16111, AlgeriaThis article demonstrates the feasibility of porous separation on the performance of displacement ventilation in a rectangular enclosure. A jet of fresh air enters the cavity through an opening at the bottom of the left wall and exits through an opening at the top of the right wall. The porous separation is placed in the center of the cavity and its height varies between 0.2 and 0.8 with three values of thickness, 0.1, 0.2, and 0.3. The heat transfer rate was calculated for different intervals of Darcy (10<sup>−6</sup> ≤ Da ≤ 10), Rayleigh (10 ≤ Ra ≤ 10<sup>6</sup>), and Reynolds (50 ≤ Re ≤ 500) numbers. The momentum and the energy equations were solved by the lattice Boltzmann method with multiple relaxation times (LB-MRT). Schemes D2Q9 and D2Q5 were chosen for the velocity and temperature fields, respectively. For porous separation, the generalized Darcy–Brinkman–Forchheimer model was adopted. It is represented by a term added in the standard LB equations. For the dynamic domain, numerical simulations revealed complex flow structures depending on all control parameters. The results showed that the thermal field, mainly in the second compartment, is very dependent on the size and permeability of the porous separation. However, they have no influence on the transfer rate.https://www.mdpi.com/2079-3197/10/1/4mixed convectionventilated cavitydisplacement ventilationporous separation
spellingShingle Zouhira Hireche
Nabil Himrane
Lyes Nasseri
Yasmine Hamrioui
Djamel Eddine Ameziani
Analysis of Thermal Performances in a Ventilated Room Using LBM-MRT: Effect of a Porous Separation
Computation
mixed convection
ventilated cavity
displacement ventilation
porous separation
title Analysis of Thermal Performances in a Ventilated Room Using LBM-MRT: Effect of a Porous Separation
title_full Analysis of Thermal Performances in a Ventilated Room Using LBM-MRT: Effect of a Porous Separation
title_fullStr Analysis of Thermal Performances in a Ventilated Room Using LBM-MRT: Effect of a Porous Separation
title_full_unstemmed Analysis of Thermal Performances in a Ventilated Room Using LBM-MRT: Effect of a Porous Separation
title_short Analysis of Thermal Performances in a Ventilated Room Using LBM-MRT: Effect of a Porous Separation
title_sort analysis of thermal performances in a ventilated room using lbm mrt effect of a porous separation
topic mixed convection
ventilated cavity
displacement ventilation
porous separation
url https://www.mdpi.com/2079-3197/10/1/4
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