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Elaf N. Mahrous

Observed names: Elaf Mahrous, Elaf N Mahrous, Mahrous, E., Mahrous, Elaf Naeem
ORCID: 0000-0002-1712-841X
Observed ORCID: 0000-0002-1712-841X
OpenAlex ID: A5002657963
A two-dimensional numerical model for the sliding motion of liquid drops by the particle finite element method
2021 · Elaf Mahrous, R. Valéry Roy, et al. · Physics of Fluids · 15
A particle finite element-based model for droplet spreading analysis
2020 · Elaf Mahrous, Alex Jarauta, et al. · Physics of Fluids · 13
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A three-dimensional numerical model for the motion of liquid drops by the particle finite element method
2022 · Elaf Mahrous, R. Valéry Roy, et al. · Physics of Fluids · 8
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Multiscale Modeling of Elastic Waves in Carbon-Nanotube-Based Composite Membranes
2024 · Elaf N. Mahrous, Muhammad A. Hawwa, et al. · Journal of Composites Science · 1
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Roughness amplification factor for contact-state-dependent topography in copper micro deep-drawn cup surfaces
2026 · Elaf N. Mahrous · Matéria (Rio de Janeiro)
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An Eulerian-PFEM Approach to Model Transient Capillary Forces on Moving Contact Lines of Spreading Liquid Drops: Applications in Hydraulic and Fluid Dynamics
2025 · Elaf N. Mahrous, Syed Yousufuddin, et al. · Journal of Engineering Research - Egypt/Journal of Engineering Research
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Numerical Analysis of Two Immiscible Fluids in Porous Media by the Multiscale and Homogenization Methods
2023 · Elaf Mahrous, Asif Hoda, et al. · Journal of Porous Media
Modeling Footprint Profiles for Different Drop-Substrate Pairs
2023 · Elaf N Mahrous · ICMAME Conference (ICMAME)
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Simulation of Droplet Spreading Dynamics by Particle Finite Element Method Based Model and Hydrodynamic Lubrication
2019 · Elaf Mahrous, R. V. Roy, et al. · Bulletin of the American Physical Society
A Continuum Model for Elastic Waves in Embedded Carbon Nanotube Composites
2009 · Elaf N. Mahrous · Research Publication Repository of King Fahd University of Petroleum and Minerals (King Fahd University of Petroleum and Minerals)
Works count: 12
Citation count: 37
H-index: 3
I10-index: 2
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