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Microfluidic Droplet-Generation Device with Flexible Walls
Controlling droplet sizes is one of the most important aspects of droplet generators used in biomedical research, drug discovery, high-throughput screening, and emulsion manufacturing applications. This is usually achieved by using multiple devices that are restricted in their range of generated dro...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10536617/ https://www.ncbi.nlm.nih.gov/pubmed/37763933 http://dx.doi.org/10.3390/mi14091770 |
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author | Yazdanparast, Sajad Rezai, Pouya Amirfazli, Alidad |
author_facet | Yazdanparast, Sajad Rezai, Pouya Amirfazli, Alidad |
author_sort | Yazdanparast, Sajad |
collection | PubMed |
description | Controlling droplet sizes is one of the most important aspects of droplet generators used in biomedical research, drug discovery, high-throughput screening, and emulsion manufacturing applications. This is usually achieved by using multiple devices that are restricted in their range of generated droplet sizes. In this paper, a co-flow microfluidic droplet-generation device with flexible walls was developed such that the width of the continuous (C)-phase channel around the dispersed (D)-phase droplet-generating needle can be adjusted on demand. This actuation mechanism allowed for the adjustment of the C-phase flow velocity, hence providing modulated viscous forces to manipulate droplet sizes in a single device. Two distinct droplet-generation regimes were observed at low D-phase Weber numbers, i.e., a dripping regime at high- and medium-channel widths and a plug regime at low-channel widths. The effect of channel width on droplet size was investigated in the dripping regime under three modes of constant C-phase flow rate, velocity, and Capillary number. Reducing the channel width at a constant C-phase flow rate had the most pronounced effect on producing smaller droplets. This effect can be attributed to the combined influences of the wall effect and increased C-phase velocity, leading to a greater impact on droplet size due to the intensified viscous force. Droplet sizes in the range of 175–913 µm were generated; this range was ~2.5 times wider than the state of the art, notably using a single microfluidic device. Lastly, an empirical model based on Buckingham’s Pi theorem was developed to predict the size of droplets based on channel width and height as well as the C-phase Capillary and Reynolds numbers. |
format | Online Article Text |
id | pubmed-10536617 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-105366172023-09-29 Microfluidic Droplet-Generation Device with Flexible Walls Yazdanparast, Sajad Rezai, Pouya Amirfazli, Alidad Micromachines (Basel) Article Controlling droplet sizes is one of the most important aspects of droplet generators used in biomedical research, drug discovery, high-throughput screening, and emulsion manufacturing applications. This is usually achieved by using multiple devices that are restricted in their range of generated droplet sizes. In this paper, a co-flow microfluidic droplet-generation device with flexible walls was developed such that the width of the continuous (C)-phase channel around the dispersed (D)-phase droplet-generating needle can be adjusted on demand. This actuation mechanism allowed for the adjustment of the C-phase flow velocity, hence providing modulated viscous forces to manipulate droplet sizes in a single device. Two distinct droplet-generation regimes were observed at low D-phase Weber numbers, i.e., a dripping regime at high- and medium-channel widths and a plug regime at low-channel widths. The effect of channel width on droplet size was investigated in the dripping regime under three modes of constant C-phase flow rate, velocity, and Capillary number. Reducing the channel width at a constant C-phase flow rate had the most pronounced effect on producing smaller droplets. This effect can be attributed to the combined influences of the wall effect and increased C-phase velocity, leading to a greater impact on droplet size due to the intensified viscous force. Droplet sizes in the range of 175–913 µm were generated; this range was ~2.5 times wider than the state of the art, notably using a single microfluidic device. Lastly, an empirical model based on Buckingham’s Pi theorem was developed to predict the size of droplets based on channel width and height as well as the C-phase Capillary and Reynolds numbers. MDPI 2023-09-15 /pmc/articles/PMC10536617/ /pubmed/37763933 http://dx.doi.org/10.3390/mi14091770 Text en © 2023 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 Yazdanparast, Sajad Rezai, Pouya Amirfazli, Alidad Microfluidic Droplet-Generation Device with Flexible Walls |
title | Microfluidic Droplet-Generation Device with Flexible Walls |
title_full | Microfluidic Droplet-Generation Device with Flexible Walls |
title_fullStr | Microfluidic Droplet-Generation Device with Flexible Walls |
title_full_unstemmed | Microfluidic Droplet-Generation Device with Flexible Walls |
title_short | Microfluidic Droplet-Generation Device with Flexible Walls |
title_sort | microfluidic droplet-generation device with flexible walls |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10536617/ https://www.ncbi.nlm.nih.gov/pubmed/37763933 http://dx.doi.org/10.3390/mi14091770 |
work_keys_str_mv | AT yazdanparastsajad microfluidicdropletgenerationdevicewithflexiblewalls AT rezaipouya microfluidicdropletgenerationdevicewithflexiblewalls AT amirfazlialidad microfluidicdropletgenerationdevicewithflexiblewalls |