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Towards the Configuration of a Photoelectrocatalytic Reactor: Part 1—Determination of Photoelectrode Geometry and Optical Thickness by a Numerical Approach
Photoelectrocatalysis has been highlighted as a tertiary wastewater treatment in the textile industry due to its high dye mineralisation capacity. However, design improvements are necessary to overcome photo-reactors limitations. The present work proposes a preliminary configuration of a photoelectr...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9322096/ https://www.ncbi.nlm.nih.gov/pubmed/35889609 http://dx.doi.org/10.3390/nano12142385 |
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author | Borrás-Jiménez, Daniel Silva-López, Wilber Nieto-Londoño, César |
author_facet | Borrás-Jiménez, Daniel Silva-López, Wilber Nieto-Londoño, César |
author_sort | Borrás-Jiménez, Daniel |
collection | PubMed |
description | Photoelectrocatalysis has been highlighted as a tertiary wastewater treatment in the textile industry due to its high dye mineralisation capacity. However, design improvements are necessary to overcome photo-reactors limitations. The present work proposes a preliminary configuration of a photoelectrocatalytic reactor to degrade Reactive Red 239 (RR239) textile dye, using computational fluid dynamics (CFD) to analyse the mass transfer rate, radiation intensity loss ([Formula: see text]), and its effect on kinetics degradation, over a photoelectrode based on a [Formula: see text] nanotube. A study to increase the space-time yield (STY) was carried out through mass transfer rate and kinetic analysis, varying the optical thickness ([Formula: see text]) between the radiation entrance and the photocatalytic surface, photoelectrode geometry, inlet flow rate, and the surface radiation intensity. The [Formula: see text] was determined using a 1D Beer–Lambert-based model, and an extinction coefficient experimentally determined by UV-Vis spectroscopy. The results show that in RR239 solutions below concentrations of 6 mg/L, a woven mesh photoelectrode and an optimal optical thickness [Formula: see text] of 1 cm is enough to keep the [Formula: see text] below 15% and maximise the mass transfer and the STY in around 110 g/m [Formula: see text]-day. |
format | Online Article Text |
id | pubmed-9322096 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-93220962022-07-27 Towards the Configuration of a Photoelectrocatalytic Reactor: Part 1—Determination of Photoelectrode Geometry and Optical Thickness by a Numerical Approach Borrás-Jiménez, Daniel Silva-López, Wilber Nieto-Londoño, César Nanomaterials (Basel) Article Photoelectrocatalysis has been highlighted as a tertiary wastewater treatment in the textile industry due to its high dye mineralisation capacity. However, design improvements are necessary to overcome photo-reactors limitations. The present work proposes a preliminary configuration of a photoelectrocatalytic reactor to degrade Reactive Red 239 (RR239) textile dye, using computational fluid dynamics (CFD) to analyse the mass transfer rate, radiation intensity loss ([Formula: see text]), and its effect on kinetics degradation, over a photoelectrode based on a [Formula: see text] nanotube. A study to increase the space-time yield (STY) was carried out through mass transfer rate and kinetic analysis, varying the optical thickness ([Formula: see text]) between the radiation entrance and the photocatalytic surface, photoelectrode geometry, inlet flow rate, and the surface radiation intensity. The [Formula: see text] was determined using a 1D Beer–Lambert-based model, and an extinction coefficient experimentally determined by UV-Vis spectroscopy. The results show that in RR239 solutions below concentrations of 6 mg/L, a woven mesh photoelectrode and an optimal optical thickness [Formula: see text] of 1 cm is enough to keep the [Formula: see text] below 15% and maximise the mass transfer and the STY in around 110 g/m [Formula: see text]-day. MDPI 2022-07-12 /pmc/articles/PMC9322096/ /pubmed/35889609 http://dx.doi.org/10.3390/nano12142385 Text en © 2022 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Borrás-Jiménez, Daniel Silva-López, Wilber Nieto-Londoño, César Towards the Configuration of a Photoelectrocatalytic Reactor: Part 1—Determination of Photoelectrode Geometry and Optical Thickness by a Numerical Approach |
title | Towards the Configuration of a Photoelectrocatalytic Reactor: Part 1—Determination of Photoelectrode Geometry and Optical Thickness by a Numerical Approach |
title_full | Towards the Configuration of a Photoelectrocatalytic Reactor: Part 1—Determination of Photoelectrode Geometry and Optical Thickness by a Numerical Approach |
title_fullStr | Towards the Configuration of a Photoelectrocatalytic Reactor: Part 1—Determination of Photoelectrode Geometry and Optical Thickness by a Numerical Approach |
title_full_unstemmed | Towards the Configuration of a Photoelectrocatalytic Reactor: Part 1—Determination of Photoelectrode Geometry and Optical Thickness by a Numerical Approach |
title_short | Towards the Configuration of a Photoelectrocatalytic Reactor: Part 1—Determination of Photoelectrode Geometry and Optical Thickness by a Numerical Approach |
title_sort | towards the configuration of a photoelectrocatalytic reactor: part 1—determination of photoelectrode geometry and optical thickness by a numerical approach |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9322096/ https://www.ncbi.nlm.nih.gov/pubmed/35889609 http://dx.doi.org/10.3390/nano12142385 |
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