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Long-Term Stability of Different Kinds of Gas Nanobubbles in Deionized and Salt Water

Nanobubbles have many potential applications depending on their types. The long-term stability of different gas nanobubbles is necessary to be studied considering their applications. In the present study, five kinds of nanobubbles (N(2), O(2), Ar + 8%H(2), air and CO(2)) in deionized water and a sal...

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Detalles Bibliográficos
Autores principales: Zhou, Yali, Han, Zhenyao, He, Chunlin, Feng, Qin, Wang, Kaituo, Wang, Youbin, Luo, Nengneng, Dodbiba, Gjergj, Wei, Yuezhou, Otsuki, Akira, Fujita, Toyohisa
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8038778/
https://www.ncbi.nlm.nih.gov/pubmed/33917489
http://dx.doi.org/10.3390/ma14071808
Descripción
Sumario:Nanobubbles have many potential applications depending on their types. The long-term stability of different gas nanobubbles is necessary to be studied considering their applications. In the present study, five kinds of nanobubbles (N(2), O(2), Ar + 8%H(2), air and CO(2)) in deionized water and a salt aqueous solution were prepared by the hydrodynamic cavitation method. The mean size and zeta potential of the nanobubbles were measured by a light scattering system, while the pH and Eh of the nanobubble suspensions were measured as a function of time. The nanobubble stability was predicted and discussed by the total potential energies between two bubbles by the extended Derjaguin–Landau–Verwey–Overbeek (DLVO) theory. The nanobubbles, except CO(2), in deionized water showed a long-term stability for 60 days, while they were not stable in the 1 mM (milli mol/L) salt aqueous solution. During the 60 days, the bubble size gradually increased and decreased in deionized water. This size change was discussed by the Ostwald ripening effect coupled with the bubble interaction evaluated by the extended DLVO theory. On the other hand, CO(2) nanobubbles in deionized water were not stable and disappeared after 5 days, while the CO(2) nanobubbles in 1 mM of NaCl and CaCl(2) aqueous solution became stable for 2 weeks. The floating and disappearing phenomena of nanobubbles were estimated and discussed by calculating the relationship between the terminal velocity of the floating bubble and bubble size.