Mohamed Rabeh Moamed Abdellatif Elsharkawy

Dr. Mohamed Rabeh Moamed Abdellatif Elsharkawy


Research Focus & Metrics

Academic Career Length

6Years (2021-Present)

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

Representative Publications

View All Publications
5 April 2023 in Radiation Physics and Chemistry
Verified
Journal Article
Closed access
WMWael M. Mohammed
Wael M. Mohammed
SAsomia Awad
somia Awad
EAEsam E. Abdel-Hady
Esam E. Abdel-Hady
Hamdy F. M. MohamedHamdy F. M. Mohamed
Hamdy F. M. Mohamed
YEYehya S. Elsharkawy
Yehya S. Elsharkawy
MEMohamed Rabeh Moamed Abdellatif Elsharkawy
Mohamed Rabeh Moamed Abdellatif Elsharkawy

17 July 2024 in Scientific Reports
Verified
Journal Article
Open access
PDF file
EAE. E. Abdel-Hady
E. E. Abdel-Hady
SHSarah H. M. Hafez
Sarah H. M. Hafez
HMHamdy F. M. Mohamed
Hamdy F. M. Mohamed
MEMohamed Rabeh Moamed Abdellatif Elsharkawy
Mohamed Rabeh Moamed Abdellatif Elsharkawy
With a rapid increase in industrial growth around the world, the demand for an entirely novel category of nanoparticles and technologies for wastewater treatment has become a key concern for environmental protection. Recently, hybrids of layered double hydroxides (LDH), particularly those containing LDH, have gained attention as potential nanoscale adsorbents for water treatment. Recent research has shown that LDH-containing composites are interesting versatile materials with the ability to be used in energy storage, photocatalysis, nanocomposites, and water treatment. In the current work, LDH-containing composites were utilized as adsorbents for the purpose of purifying water. The adsorbents investigated are Zn–Co–Fe/LDH/Chitosan-in situ sample preparation (LDH/CS1) and Zn–Co–Fe/LDH/Chitosan-ex situ sample preparation (LDH/CS2). Furthermore, LDH/CS1 and LDH/CS2 were investigated for wastewater treatment from methyl orange dye (MO) with various adsorption conditions. When the initial MO concentration was 20 mg/L and the amount of adsorbent was 0.1 g, the removal efficiency reached 72.8 and 91.7% for LDH/CS1 and LDH/CS2, respectively. The MO’s maximum adsorption capabilities are 160.78 and 165.89 mg/g for LDH/CS1 and LDH/CS2, respectively, which is much greater than that of comparable commercial adsorbents. MO adsorption onto LDH/CS1 and LDH/CS2 was best characterized by the pseudo-second-order kinetic model. The equilibrium adsorption data was followed by the Freundlich and Langmuir models. The adsorption is favorable as evidenced by the equilibrium parameter RL values for MO adsorption onto LDH/CS1 and LDH/CS2, which were 0.227 and 0.144, respectively. Using the free volume distribution method and the positron annihilation lifetime technique, the nanostructure of the materials was examined.

21 April 2022 in Polymers
Verified
Journal Article
Open access
PDF file
MGMahmoud Gomaa
Mahmoud Gomaa
ASArturo Sánchez-Ramos
Arturo Sánchez-Ramos
NUNieves Ureña
Nieves Ureña
María T. Pérez-PriorMaría T. Pérez-Prior
María T. Pérez-Prior
BLBelen Levenfeld
Belen Levenfeld
MEMohamed Rabeh Moamed Abdellatif Elsharkawy
Mohamed Rabeh Moamed Abdellatif Elsharkawy
Free volume plays a key role on transport in proton exchange membranes (PEMs), including ionic conduction, species permeation, and diffusion. Positron annihilation lifetime spectroscopy and electrochemical impedance spectroscopy are used to characterize the pore size distribution and ionic conductivity of synthesized PEMs from polysulfone/polyphenylsulfone multiblock copolymers with different degrees of sulfonation (SPES). The experimental data are combined with a bundle-of-tubes model at the cluster-network scale to examine water uptake and proton conduction. The results show that the free pore size changes little with temperature in agreement with the good thermo-mechanical properties of SPES. However, the free volume is significantly lower than that of Nafion®, leading to lower ionic conductivity. This is explained by the reduction of the bulk space available for proton transfer where the activation free energy is lower, as well as an increase in the tortuosity of the ionic network.

8 December 2021 in Polymers for Advanced Technologies
Verified
Journal Article
Closed access
PDF file
MEMohamed Rabeh Moamed Abdellatif Elsharkawy
Mohamed Rabeh Moamed Abdellatif Elsharkawy
Hamdy F. M. MohamedHamdy F. M. Mohamed
Hamdy F. M. Mohamed
MHMohamed H. M. Hassanien
Mohamed H. M. Hassanien
MGMahmoud Gomaa
Mahmoud Gomaa

4 June 2025 in International Journal of Hydrogen Energy
Verified
Journal Article
Open access
MGMahmoud Gomaa
Mahmoud Gomaa
IRIñaki Requena
Iñaki Requena
MEMohamed Rabeh Moamed Abdellatif Elsharkawy
Mohamed Rabeh Moamed Abdellatif Elsharkawy
MRManuel A. Rodrigo
Manuel A. Rodrigo
Justo LobatoJusto Lobato
Justo Lobato

3 January 2026 in Nature Communications
Verified
Journal Article
Open access
PDF file
DKDavid J. Keeble
David J. Keeble
THTheodore D. C. Hobson
Theodore D. C. Hobson
JWJulia Wiktor
Julia Wiktor
EBEthan Berger
Ethan Berger
MDMarcel Dickmann
Marcel Dickmann
KDKen Durose
Ken Durose
Antimony selenide (Sb 2 Se 3 ) has an optimal bandgap and absorption coefficient for thin film solar cell applications and comprises earth abundant elements. The rate of increase in reported power conversion efficiencies has slowed due to a persistently large open circuit voltage deficit attributed to detrimental concentrations of point defects. Here we use depth-profiling positron annihilation lifetime spectroscopy to study Sb 2 Se 3 crystals and thin films. The method is specific to neutral and negative charge states of vacancy-related defects. Both monovacancy and divacancy defects are identified in intrinsic and n-type samples but no monovacancy defects are detected in the p-type sample. Comparison of the experimental positron lifetimes with density functional theory calculated values provide evidence for the observation of Sb monovacancies in the –3 state and of Se monovacancies in the –2 state. The results are consistent with recent density function theory predictions that the Sb and the Se monovacancy defects both have accessible negative charge states.