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A hydrophilic carbon foam/molybdenum disulfide composite as a self-floating solar evaporator

Solar-driven interfacial evaporation has gained increasing attention as an emerging and sustainable technology for wastewater treatment and desalinization. The carbon/molybdenum disulfide (C/MoS(2)) composite has attracted more attention due to its outstanding light absorption capability and optoele...

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Detalles Bibliográficos
Autores principales: Mohseni Ahangar, Ali, Hedayati, Mohammad Ali, Maleki, Mahdi, Ghanbari, Hajar, Valanezhad, Alireza, Watanabe, Ikuya
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9832982/
https://www.ncbi.nlm.nih.gov/pubmed/36712601
http://dx.doi.org/10.1039/d2ra07810d
Descripción
Sumario:Solar-driven interfacial evaporation has gained increasing attention as an emerging and sustainable technology for wastewater treatment and desalinization. The carbon/molybdenum disulfide (C/MoS(2)) composite has attracted more attention due to its outstanding light absorption capability and optoelectronic properties as a solar steam generator. However, the hydrophobic nature of carbon and MoS(2)-based materials hinders their wettability, which is crucial to the effective and facile operation of a solar generator of steam. Herein, a pH-controlled hydrothermal method was utilized to deposit a promising photothermal MoS(2) coating on melamine-derived carbon foams (CFs). The hydrophilic CF/MoS(2) composite, which can easily be floatable on the water surface, is a high-efficiency solar steam evaporator with a rapid increase in temperature under photon irradiation. Due to the localized heat confinement effect, the self-floating composite foam on the surface of water has the potential to produce a significant temperature differential. The porous structure effectively facilitates fast water vapor escape, leading to an impressively high evaporation efficiency of 94.5% under a light intensity of 1000 W m(−2).