Walid Foudhil

Dr. Walid Foudhil

University of Carthage, Faculty of Sciences of Bizerte, Tunis, Tunisia
orcid

Research Focus & Metrics

Academic Career Length

7Years (2020-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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20 April 2021 in Heat and Mass Transfer
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Journal Article
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Walid FoudhilWalid Foudhil
Walid Foudhil
PCPin Chen
Pin Chen
KFKamel Fahem
Kamel Fahem
SHSouad Harmand
Souad Harmand
SJSadok Ben Jabrallah
Sadok Ben Jabrallah

1 May 2020 in International Journal of Thermal Sciences
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Journal Article
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DKDorra Khilifi
Dorra Khilifi
Walid FoudhilWalid Foudhil
Walid Foudhil
SHSouad Harmand
Souad Harmand
SJSadok Ben Jabrallah
Sadok Ben Jabrallah

31 January 2020 in Journal of Thermal Analysis and Calorimetry
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NGNihel Grich
Nihel Grich
Walid FoudhilWalid Foudhil
Walid Foudhil
SHSouad Harmand
Souad Harmand
SJSadok Ben Jabrallah
Sadok Ben Jabrallah

4 January 2023 in Heat Transfer Engineering
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Journal Article
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Walid FoudhilWalid Foudhil
Walid Foudhil
DKDorra Khilifi
Dorra Khilifi
YDYvan Dutil
Yvan Dutil
SHSouad Harmand
Souad Harmand
SJSadok Ben Jabrallah
Sadok Ben Jabrallah
In this work, a three-dimensional numerical simulation, accompanied by an experimental study, of the evaporation of one or more nonaligned liquid droplets deposited on a solid substrate and surrounded by air was produced. In addition to the central droplet, the behavior of other neighboring droplets was tracked. Evaporation of a single droplet S was compared with that of multiple droplets (a droplet C surrounded by four non-aligned droplets). The shielding effect exerted by the four droplets on the droplet C increases the life of the latter by 83% as compared to a single droplet. Evaporated flow of the droplet C is reduced by 58% compared to the case of the isolated droplet S. The droplets at the extremities evaporate faster (compared to the droplet C, the evaporated volume can increase up to 57%), since they have less interaction with nearby droplets. A geometric coefficient F characterizing the ratio of the distance separating two neighboring droplets, to the diameter of a droplet was introduced. The shielding effect decreases with the increase of F. For F greater than 5, the behavior of the extremity droplets tends towards that of a single droplet.

17 October 2023 in Journal of Thermal Engineering
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STSoumaïla Tigampo
Soumaïla Tigampo
SKSami Kooli
Sami Kooli
NSNizar Ben Salah
Nizar Ben Salah
Walid FoudhilWalid Foudhil
Walid Foudhil
REReda Errais
Reda Errais
VSVincent Sambou
Vincent Sambou
In this work, we present the validation of a numerical model of a greenhouse thermally in-sulated on three sides with a tomato crop. A CFD software (Ansys-Fluent) was used to solve the numerical model. The discrete ordinate model was included to solve the radiative trans-fer equation. The results of the numerical model were compared with the values of air tem-perature observations at different points in the greenhouse. Good agreement was obtained between the simulated and measured values, with coefficients of determination R2 = 0.77, R2 = 0.84, R2 = 0.99, and R2 = 0.89 for the temperatures of the points 10 cm, 80 cm, and 210 cm above the ground and the average temperature in the greenhouse, respectively. A third-order polynomial curve was drawn between the simulated and measured values of relative humidity in the greenhouse. These R2 values are 0.9786 and 0.7165, the simulated and measured relative humidity, respectively. The simulation results showed low velocity values with an average of 0.525 m/s located between 1.5 m and 2 m from the ground.

22 May 2022 in Water
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Journal Article
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Walid FoudhilWalid Foudhil
Walid Foudhil
Costanza AricòCostanza Aricò
Costanza Aricò
PPPatrick Perré
Patrick Perré
Faculte des sciences de BizerteFaculte des sciences de Bizerte
Faculte des sciences de Bizerte
The present work presents a numerical study of the evaporation of a sessile liquid droplet deposited on a substrate and subjected to different heating configurations. The physical formulation accounts for evaporation, the Marangoni effect, conductive transfer in the support, radiative heating, and diffusion–convection in the droplet itself. The moving interface is solved using the Arbitrary Lagrangian–Eulerian (ALE) method. Simulations were performed using COMSOL Multiphysics. Different configurations were performed to investigate the effect of the heating conditions on the shape and intensity of the Marangoni circulations. A droplet can be heated by the substrate (different natures and thicknesses were tested) and/or by a heat flux supplied at the top of the droplet. The results show that the Marangoni flow can be controlled by the heating configuration. An upward Marangoni flow was obtained for a heated substrate and a downward Marangoni flow for a flux imposed at the top of the droplet. Using both heat sources generated two vortices with an upward flow from the bottom and a downward flow from the top. The position of the stagnation zone depended on the respective intensities of the heating fluxes. Controlling the circulation in the droplet might have interesting applications, such as the control of the deposition of microparticles in suspension in the liquid, the deposition of the solved constituent, and the enhancement of the evaporation rate.